9th Edition of the Large Hadron Collider Physics Conference

7 Jun 2021, 12:00 → 12 Jun 2021, 16:35 Europe/Paris

Zoom

Tulika Bose (University of Wisconsin Madison (US)), Dave Charlton (University of Birmingham (GB)), Giovanni Marchiori (APC, IN2P3 and Université de Paris (Paris, France)), Roberto Salerno (Centre National de la Recherche Scientifique (FR))

The Ninth Annual Large Hadron Collider Physics (LHCP2021) conference is planned in Paris online from 7th to 12th June 2021

---

NEWS (03/11/2021): the LHCP2021 proceedings have been reviewed and are now available  at this URL: https://pos.sissa.it/397/

NEWS (18/10/2021): the LHCP2021 proceedings are currently under review and will appear at this URL: https://pos.sissa.it/397/

NEWS (12/06/2021): the winners of the poster awards and the site selected to host LHCP 2023 have been announced in the closing plenary session

NEWS (28/04/2021): the second bulletin is now available on the conference website (click here)

NEWS (23/04/2021): poster abstracts have been reviewed and acceptance notifications have been sent by e-mail. Information about the poster and poster session formats are available here. More detailed instructions will be sent to the poster presenters by e-mail.

NEWS (22/04/2021): thanks to CERN and IUPAP sponsorships, no fees are required to participate to the LHCP2021 conference. Participants attending the online conference are required to register in order to receive by e-mail the instructions for the video connections.

---

    The LHCP conference series started in 2013 after a successful fusion of two international conferences, "Physics at Large Hadron Collider Conference" and "Hadron Collider Physics Symposium". The conference programme will be devoted to a detailed review of the latest experimental and theoretical results on collider physics, and recent results of the LHC Run II, and discussions on further research directions within the high energy particle physics community including both theory and experiment sides. The main goal of the conference is to provide intense and lively discussions between experimentalists and theorists in research areas such as the Standard Model Physics and Beyond, the Higgs Boson, Supersymmetry, Heavy Quark Physics and Heavy Ion Physics as well as the recent progress in the high luminosity upgrades of the LHC and future colliders developments.

With great regret we have concluded that the 9th LHCP conference, to be held 7-12 June 2021, will need to be fully online, due to the Covid-19 pandemic and its uncertainties.

The conference will be maintained for the same days, with an adjusted timetable to improve remote participation from around the world, similar to that of the 2020 edition of LHCP. 

---

 

MAIN DEADLINES

Registration
- opening	12 December 2020
- closing	2 June 2021
Poster abstract submission
- submission deadline	19 April 2021
- acceptance notification	23 April 2021 at the latest
Start of the conference	7 June 2021 12:00
Proceedings submission	20 September 2021

LCHP2021 posters - Presenter availability.pdf

LHCP2021_1stBulletin.pdf

LHCP2021_2ndBulletin.pdf

LHCP2021_online_poster.pdf

LHCP2021 stats.pdf

Monday 7 June

Opening Plenary: Highlights from LHC and Experiments

Conveners: Giovanni Marchiori (APC, IN2P3 and Université de Paris (Paris, France)), Tulika Bose (University of Wisconsin Madison (US))

1 Welcome from the LOC

Speakers: Giovanni Marchiori (APC, IN2P3 and Université de Paris (Paris, France)), Roberto Salerno (Centre National de la Recherche Scientifique (FR))

LHCP2021_Opening.pdf

Recording

2 The European Strategy for Particle Physics and CERN's future

Speaker: Fabiola Gianotti (CERN)

LHCP-Gianotti.pdf

LHCP-Gianotti.ppt

Recording

3 Status of the LHC

Speaker: Mike Lamont (CERN)

LHC-status-LHCP-June21.pdf

Recording

4 Highlights and perspectives from the ALICE experiment

Speaker: Mateusz Ploskon (Lawrence Berkeley National Lab. (US))

LHCP2021-ALICE-Overview_v2.0.pdf

Recording

13:25 Coffee break

Opening Plenary: Highlights from LHC and Experiments II

Conveners: Bruno Mansoulie (Université Paris-Saclay (FR)), Roberto Salerno (Centre National de la Recherche Scientifique (FR))

5 Highlights and perspectives from the ATLAS experiment

Speaker: Manuella Vincter (Carleton University (CA))

Recording

talk_LHCP21_Vincter.pdf

6 Highlights and perspectives from the CMS experiment

Speaker: Gautier Hamel de Monchenault (IRFU, CEA, Université Paris-Saclay (FR))

GHM_LHCP2021_CMS-Highlights.pdf

Recording

7 Highlights and perspectives from the LHCb experiment

Speaker: Chris Parkes (University of Manchester (GB))

LHCb_LHCP_Parkes_070621.pdf

Recording

8 Report on Diversity, Inclusion and Outreach activities at LHC

Speaker: Brajesh Choudhary (University of Delhi (IN))

LHCP2021-DIO-Talk-BCC-7June2021.pdf

Recording

15:05 Coffee break

TeV-scale BSM: General BSM

Conveners: Dr Carl Gwilliam (University of Liverpool (GB)), Seema Sharma (Indian Institute of Science Education and Research (IN)), Yael Shadmi (Technion)

9 ATLAS + CMS searches beyond inclusive resonances in leptonic final states

Speaker: Tadej Novak (Deutsches Elektronen-Synchrotron (DE))

LHCP_searches_leptons_ATLAS+CMS.pdf

Recording

10 ATLAS + CMS Searches beyond inclusive resonances in hadronic final states

Speaker: Alberto Orso Maria Iorio (Universita e sezione INFN di Napoli (IT))

CMS_Atlas_Beyond_resonant_hadronic_Iorio.pdf

Recording

11 ATLAS + CMS Searches for Di-/Tri-boson resonances

Speaker: Antonis Agapitos (Peking University (CN))

LHCP_Resonant_Multiboson_Searches_7_6_21_v4.pdf

Recording

12 Global searches for new physics based on novel event characteristics

Speaker: Cari Cesarotti (Harvard University)

isotropyLHCP2021.pdf

Recording

13 Discussion

BSM - Feebly Interacting Particles: Neutral FIPs and other current experiments

Conveners: Emma Torro Pastor (Univ. of Valencia and CSIC (ES)), José Francisco Zurita (IFIC - Univ. of Valencia and CSIC (ES)), Niki Saoulidou (National and Kapodistrian University of Athens (GR)), Dr Vasiliki Mitsou (Univ. of Valencia and CSIC (ES)), Xabier Cid Vidal (Instituto Galego de Física de Altas Enerxías)

14 Searches for long-lived particles and Heavy Neutral Leptons: Theory perspective

Speaker: Giovanna Cottin (Universidad Adolfo Ibañez)

LHCPC2021_HNLsLLPs_GCOTTIN.pdf

Recording

15 Heavy Neutral Lepton searches at the LHC

Speaker: Matthias Komm (CERN)

mkomm_2021_06_06_LHCP.pdf

Recording

16 Large radius tracking and displaced vertex searches at the LHC

Speaker: Carlos Vazquez Sierra (CERN)

CVS_LLPs_LHCP21_v3.pdf

Recording

17 Searches for displaced and delayed signatures at the LHC

Speaker: Rachel Christine Rosten (Ohio State University (US))

2021_06_07_LHCP_LLP.pdf

Recording

18 Searches in current non-LHC experiments

Speaker: Prof. Christopher Hearty (University of British Columbia (CA))

Recording

Search for FIPs at non-LHC experiments 7-Jun-2021.pdf

Electroweak physics: VBS/VBF

Conveners: Davide Pagani (Deutsches Elektronen-Synchrotron (DE)), Hang Yin (Central China Normal University CCNU (CN)), Joany Manjarres (Technische Universitaet Dresden (DE)), Dr Pietro Vischia (Universite Catholique de Louvain (UCL) (BE))

19 VBS/VBF (theory)

Speaker: Dr Alexander Karlberg (University of Oxford)

070621LHCP2021.pdf

Recording

20 VBS/VBF measurements (without photons) at ATLAS

Speaker: Karolos Potamianos (University of Oxford (GB))

2021-06-07-LHCP-Potamianos.pdf

Recording

21 VBS/VBF measurements (without photons) at CMS

Speaker: Matteo Presilla (Universita e INFN, Padova (IT))

LHCP2021_VBS_CMS.pdf

Recording

22 VBS/VBF measurements (with photons) at ATLAS and CMS

Speaker: Ben Harry Smart (Science and Technology Facilities Council STFC (GB))

LHCP2021_ATLAS_CMS_VBS_VBF_ZyWy_photons_Ben_Smart_7_6_21_v2.pdf

Higgs physics: Session 1

Conveners: Giuliano Panico (University of Florence and INFN Florence), Kerstin Tackmann (Deutsches Elektronen-Synchrotron (DE)), Meng Xiao (ZJU - Zhejiang University (CN))

23 Higgs decays to bosons at ATLAS+CMS

Speaker: Sana Ketabchi (University of Toronto (CA))

LHCP21_HtoBosons_vfinal.pdf

Recording

24 Higgs decays to third-generation fermions at ATLAS+CMS

Speaker: Christina Reissel (ETH Zurich (CH))

Recording

Reissel_LHCP_HiggstoThirdGenFermions_final.pdf

25 Higgs CP studies at ATLAS+CMS

Speaker: Maria Moreno Llacer (Univ. of Valencia and CSIC (ES))

MariaMorenoLlacer_HiggsCP_ATLASandCMS_June2021.pdf

Recording

26 Rare Higgs decays at ATLAS+CMS

Speaker: Kajari Mazumdar (Tata Inst. of Fundamental Research (IN))

lhcp.pdf

Recording

Detector performance: Session 1

Conveners: Francesco Prino (Universita e INFN Torino (IT)), Nicole Skidmore (University of Bonn (DE)), Nora Emilia Pettersson (CERN), Phat Srimanobhas (Chulalongkorn University (TH))

27 Highlight: ATLAS

Speaker: Davide Cieri (Max-Planck-Institut fur Physik (DE))

2021_06_07_LHCP2021_ATLAS_performance.pdf

Recording

28 Highlight: CMS-TOTEM

Speaker: Laurent Forthomme (Helsinki Institute of Physics (FI))

lhcp_cmstotem_forthomme.pdf

29 Highlight: ALICE: reconstruction and TPC calibration in Run 3

Speaker: Ernst Hellbar (GSI - Helmholtzzentrum fur Schwerionenforschung GmbH (DE))

20210607_ALICETPCRecoCalib.pdf

Recording

30 HIghlight: LHCb

Speaker: Louis Henry (CERN)

LouisHenry_LHCbTrigger.pdf

Recording

31 Highlight: Forward Physics (LHCf + FASER)

Speaker: Eugenio Berti (Universita e INFN, Firenze (IT))

EBerti_LHCP2021.pdf

Recording

QCD: Jet substructure and correlations in hadronic final States

Conveners: Ben Nachman (Lawrence Berkeley National Lab. (US)), Prof. Frank Petriello (Northwestern University and Argonne National Lab), Gabor Veres (Eotvos Lorand University (HU)), Joe Osborn (Oak Ridge National Laboratory), Laura Brittany Havener (Yale University (US))

32 Recent progress in jet substructure calculations

Speaker: Daniel Reichelt

LHCP2021_DReichelt.pdf

Recording

33 Jet Substructure + Correlations in Hadronic Final States from CMS

Speaker: Markus Seidel (University of Maryland (US))

lhcp_mseidel.pdf

Recording

34 Jet Substructure + Correlations in Hadronic Final States from ATLAS

Speaker: Robin Newhouse (University of British Columbia (CA))

LHCP 2021 - Jet Substructure + Correlations in Hadronic Final States from ATLAS - Robin Newhouse (3).pdf

Recording

35 Jet Substructure + Correlations in Hadronic Final States from ALICE

Speaker: James Mulligan (University of California, Berkeley (US))

Mulligan_LHCP.pdf

Recording

Top physics: Top production

Conveners: Gauthier Durieux (CERN), Jose Enrique Palencia Cortezon (Universidad de Oviedo (ES)), Maria Moreno Llacer (Univ. of Valencia and CSIC (ES)), Stephen Farry (University of Liverpool (GB))

Top@LHCP2021.pdf

36 Theory status of Top Production

Speaker: Anna Kulesza (University of Muenster)

lhcp21_ak.pdf

lhcp21_ak.pptx

Recording

37 Recent Results in Top Pair Production Measurements at the LHC

Speaker: Michele Faucci Giannelli (INFN e Universita Roma Tor Vergata (IT))

Michele Faucci Giannelli, Top pair production at the LHC.pptx

Recording

38 Recent Results in Single Top Production at the LHC

Speaker: Galo Rafael Gonzalvo Rodriguez (Univ. of Valencia and CSIC (ES))

LHCP Single Top.pdf

Recording

39 Associated Top Production at the LHC

Speaker: Barbara Alvarez Gonzalez (Universidad de Oviedo (ES))

LHCP2021_BarbaraAlvarez_final.pdf

Recording

40 Four Top Production at the LHC

Speaker: Albert Kong (University of Adelaide (AU))

lhcp2021-talk.pdf

Recording

16:45 Coffee break

Heavy ions: Quarkonium, exotics and other bound states

Conveners: Dr Alexander Rothkopf (University of Stavanger), Hengne Li (South China Normal University (CN)), Maximiliano Puccio (CERN), Qipeng Hu (Lawrence Livermore Nat. Laboratory (US)), Wei Li (Rice University (US))

41 Jets and Quarkonium as open-quantum systems

Speaker: Dr Xiaojun Yao (Massachusetts Institute of Technology)

lhcp.pdf

Recording

42 New measurements in the quarkonia sector with focus on new discriminatory observables

Speaker: Minjung Kim (Ruprecht Karls Universitaet Heidelberg (DE))

LHCP2021_mjkim_final.pdf

Recording

43 X(3872) and exotic quarkonia production in heavy-ion

Speaker: Guillaume Falmagne

LHCP 07.06.2021.pdf

Recording

44 X(3872) and exotic quarkonia production in small systems

Speaker: John Matthew Durham (Los Alamos National Laboratory)

LHCP_Durham.pdf

Recording

45 (Anti)(Hyper)nuclei production at the LHC

Speaker: Luca Barioglio (Technische Universitaet Muenchen (DE))

LHCP21_Barioglio_v4.pdf

Recording

46 Loosely bound state production

Speaker: Kfir Blum

LHCP2021 hypertriton.pdf

Recording

Joint sessions: BSM and Higgs physics

Conveners: Carl Gwilliam (University of Liverpool (GB)), Kerstin Tackmann (Deutsches Elektronen-Synchrotron (DE)), Xabier Cid Vidal (Instituto Galego de Física de Altas Enerxías)

LHC_JointHiggsTop.pdf

47 BSM Higgs decays at ATLAS+CMS

Speaker: Javier Montejo Berlingen (CERN)

20210607_HBSM_LHCP_v2.pdf

Recording

48 Exotic Higgs decays (theory)

Speaker: Elina Fuchs (Fermilab and University of Chicago)

49 H->inv at ATLAS+CMS

Speaker: Andreas Albert (Boston University (US))

2021-06-07_lhcp.pdf

Recording

50 Searches for additional Higgs bosons at ATLAS+CMS

Speaker: Junquan Tao (Institute of High Energy Physics, Chinese Academy of Sciences (CN))

LHCP2021_AdditionalHiggsAtLHC_JTao.pdf

Recording

51 Discussion

QCD: Nucleon Structure and Soft QCD

Conveners: Ben Nachman (Lawrence Berkeley National Lab. (US)), Frank Petriello (Northwestern University and Argonne National Lab), Gabor Veres (Eotvos Lorand University (HU)), Joe Osborn (Oak Ridge National Laboratory), Laura Brittany Havener (Yale University (US))

52 Recent theoretical progress in nuclear structure

Speaker: Maria Pia Zurita

LHCP2021_v2.pdf

Recording

53 Nucleon Structure and Soft QCD from CMS

Speaker: Rajat Gupta (Panjab University (IN))

LHCP2021_SoftQCDCMS_Rajat_v1.pdf

Recording

54 Nucleon Structure and Soft QCD from ATLAS

Speaker: Andre Sopczak (Czech Technical University in Prague (CZ))

Recording

Sopczak_LHCP2021_final.pdf

55 Nucleon Structure and Soft QCD from LHCb

Speaker: Agnieszka Oblakowska-Mucha (AGH University of Science and Technology (PL))

Recording

SoftQCD_AMucha_LHCP2022.pdf

56 Nucleon Structure and Soft QCD from ALICE

Speaker: Sushanta Tripathy (Universita e INFN, Bologna (IT))

Recording

SoftQCD-ALICE-Sushanta.pdf

57 The first experimental observation of the Odderon

Speaker: Frigyes Janos Nemes (CERN (also at Wigner RCP Budapest, Hungary))

LHCP_2021_Frigyes_Nemes_v2 (3).pdf

Recording

Tools: Theory tools

Conveners: Andy Buckley (University of Glasgow (GB)), Loukas Gouskos (CERN), Philip Ilten (University of Cincinnati (US)), Sandro Christian Wenzel (CERN), Stefano Carrazza (CERN)

58 High precision calculations

Speaker: Tobias Neumann (Brookhaven National Laboratory)

Neumann_Tobias_LHCP2021.pdf

Recording

59 Lattice developments and tools

Speaker: Huey-Wen Lin

Lattice developments and tools

Recording

60 Event generation techniques and tools

Speaker: Marek Schoenherr (University of Durham (GB))

MarekSchoenherr_MCCompChallenges.pdf

Recording

61 BSM develoments and tools

Speaker: Dr Tomas Gonzalo (Monash University)

Recording

TomasGonzaloLHCP2021.pdf

62 Discussion

Top physics: Interpretations in final state states with top quark

Conveners: Gauthier Durieux (CERN), Jose Enrique Palencia Cortezon (Universidad de Oviedo (ES)), Maria Moreno Llacer (Univ. of Valencia and CSIC (ES)), Stephen Farry (University of Liverpool (GB))

Top@LHCP2021.pdf

63 Bayesian inference and unsupervised ML @ Four-tops

Speaker: Ezequiel Alvarez de los Alvarez de San Luis

Corner-plot for Bayesian Inference algorithm 500fb-1

Ezequiel_Alvarez_lhcep2021.pdf

Recording

64 BSM reach of single top-quark measurements

Speaker: Dr Alberto Tonero (Carleton University)

Recording

slides.pdf

65 BSM searches with top final states

Speaker: Junpei Maeda (Kobe University (JP))

BSMwTop_LHCP_2021-06-07_final.pdf

Recording

66 EFT Results from ATLAS

Speaker: Laura Barranco Navarro (Stockholm University (SE))

LHCPBarranco.pdf

Recording

67 EFT Results from CMS

Speaker: Juan Gonzalez (Universidad de Oviedo (ES))

LHCP2021_Jgonzalez.pdf

Upgrades: Physics at HL-LHC

Conveners: Christian Ohm (KTH Royal Institute of Technology (SE)), LianTao Wang (University of Chicago), Magnus Mager (CERN), Saptaparna Bhattacharya (Northwestern University (US)), Silvia Borghi (University of Manchester (GB))

LHCPInstructions.pdf

68 Physics prospects ALICE in Run 5 and beyond

Speaker: Antonio Uras (Centre National de la Recherche Scientifique (FR))

Alice3_LCHP2021_Uras.pdf

Recording

69 Physics with precision timing at HL-LHC with ATLAS and CMS

Speaker: Christian Ohm (KTH Royal Institute of Technology (SE))

Ohm_HGTD_LHCP2021.pdf

Recording

70 Boosting the physics potential of the HL-LHC ATLAS and CMS experiments with new trigger systems

Speaker: Swagata Mukherjee (Rheinisch Westfaelische Tech. Hoch. (DE))

LHCP2021_SM.pdf

Recording

71 Physics prospects for LHCb upgrade II

Speaker: Francesca Dordei (INFN, Cagliari (IT))

Recording

upgrade_II.pdf

72 Testing BSM physics at the HL-LHC

Speaker: stefania gori (UC Santa Cruz)

Recording

TalkLHCp.pdf

Tuesday 8 June

Plenary I: Top Physics

Conveners: Benjamin Fuks (Centre National de la Recherche Scientifique (FR)), Klaus Monig (Deutsches Elektronen-Synchrotron (DE))

73 Theoretical aspects of top physics

Speaker: Malgorzata Maria Worek (Rheinisch Westfaelische Tech. Hoch. (DE))

Recording

TopPhysics-MWorek.pdf

74 Results on tt+X production

Speaker: Joshuha Thomas-Wilsker (Chinese Academy of Sciences)

Recording

Results_on_ttX_Production_JTW.pdf

75 Top production and decay

Speaker: Sven Menke (Max-Planck-Institut fur Physik (DE))

lhcp2021.pdf

Recording

76 Rare production and decay processes

Speaker: Carlo Alberto Gottardo (NIKHEF, Radboud University (Nijmegen))

RareTop_Gottardo_LHCP2021.pdf

Recording

14:00 Coffee break

TeV-scale BSM: SUSY

Conveners: Carl Gwilliam (University of Liverpool (GB)), Seema Sharma (Indian Institute of Science Education and Research (IN)), Yael Shadmi (Technion)

77 ATLAS + CMS Searches for squarks and gluinos

Speaker: Stefio Yosse Andrean (Stockholm University (SE))

LHCP2021_gluino_squark_Yosse.pdf

Recording

78 ATLAS + CMS Searches for EWK SUSY in hadronic and semi-leptonic final states

Speaker: Stefan Guindon (CERN)

LHCP_EWKSUSY_Guindon.pdf

Recording

79 ATLAS + CMS Searches for EWK SUSY in fully leptonic and soft final states

Speaker: Christian Herwig (Fermi National Accelerator Lab. (US))

herwig_v1.pdf

Recording

80 The current state of SUSY and ways forward

Speaker: Matthew Reece (Harvard University)

Recording

Reece_LHCP_SUSY_2021.pdf

81 Discussions

BSM - Feebly Interacting Particles: Dark Photons and ALPs; Future experiments

Conveners: Emma Torro Pastor (Univ. of Valencia and CSIC (ES)), José Francisco Zurita, Niki Saoulidou (National and Kapodistrian University of Athens (GR)), Vasiliki Mitsou (Univ. of Valencia and CSIC (ES)), Xabier Cid Vidal (Instituto Galego de Física de Altas Enerxías)

82 Theoretical overview of ALPs and Dark Photons

Speaker: Patrick Foldenauer

lhcp21_foldenauer.pdf

Recording

83 Searches for ALPs at the LHC

Speaker: Kristof Schmieden (Johannes Gutenberg Universitaet Mainz (DE))

2021-06_LHCP_ALPsAtLHC.pdf

Recording

84 Searches for Dark Photons at the LHC

Speaker: Federico Leo Redi (EPFL - Ecole Polytechnique Federale Lausanne (CH))

LHCP_DP_CINCO_Redi_2021_v1.0.pdf

Recording

85 Status of FASER and MAPP

Speaker: Candan Dozen (Tsinghua University (CN))

LHCP2021_FASER(nu)_MAPP_SND.pdf

Recording

86 Future LLP experiments

Speaker: Heather Russell (CERN)

20210608_hrussell_LHCP.pdf

Recording

Electroweak physics: Diboson/multiboson

Conveners: Davide Pagani (Deutsches Elektronen-Synchrotron (DE)), Hang Yin (Central China Normal University CCNU (CN)), Joany Manjarres (Technische Universitaet Dresden (DE)), Pietro Vischia (Universite Catholique de Louvain (UCL) (BE))

87 Polarized multiboson production at the LHC and beyond

Speaker: Richard Ruiz (Institute of Nuclear Physics (IFJ) PAN)

Recording

rruiz_LHCP2021_MuliVPolar.pdf

88 Multiboson measurements (not photon-induced) at ATLAS

Speaker: Sabine Wedam Lammers (Indiana University (US))

Multiboson_LHCP.pdf

Recording

89 Multiboson measurements (not photon-induced) at CMS

Speaker: Alicia Calderon Tazon (Universidad de Cantabria and CSIC (ES))

Multibosons_CMS_LHCP2021_v2.pdf

Recording

90 Photon-induced processes [theory]

Speaker: Marta Luszczak (University of Rzeszow)

Luszczak-M-LHCP2021.pdf

Recording

91 Photon-induced processes at ATLAS and CMS

Speaker: Christophe Royon (The University of Kansas (US))

lhcp2021.pdf

Recording

Flavour physics: Session 1

Conveners: Diego Guadagnoli (LAPTh Annecy), Dmytro Kovalskyi (Massachusetts Inst. of Technology (US)), Michel De Cian (EPFL - Ecole Polytechnique Federale Lausanne (CH)), Sarah Porteboeuf (Université Clermont Auvergne (FR)), Semen Turchikhin (Joint Institute for Nuclear Research (RU))

92 Theory lessons from flavour data

Speaker: Claudia Cornella (U. Zurich)

LHCp_Cornella.pdf

Recording

93 SM challenges

Speaker: Javier Virto (Universitat de Barcelona)

Recording

TALK___Theory_Challenges_in_exclusive_rare_B_decays__LHCP2021_.pdf

94 Rare decays in b→s/d sector

Speaker: Yanting Fan (University of Chinese Academy of Sciences (CN))

LHCP2021_rareb2sd.pdf

Recording

95 b → c status and prospects with focus on ratio observables

Speaker: Alessandra Gioventu (Universidade de Santiago de Compostela (ES))

LHCP_b2c_Gioventu_v4.pdf

Recording

96 Bs → mumu status and prospects

Speaker: Jacco Andreas De Vries (Universiteit Maastricht (NL))

jacco_LHCP-bsmumu_080621_v6.pdf

Recording

Higgs physics: Session 2

Conveners: Giuliano Panico (University of Florence and INFN Florence), Kerstin Tackmann (Deutsches Elektronen-Synchrotron (DE)), Meng Xiao (ZJU - Zhejiang University (CN))

97 Higgs combination at ATLAS+CMS

Speaker: Haider Abidi (Brookhaven National Laboratory (US))

HiggsCombination.pdf

Recording

98 Higgs EFT benchmarks -- CANCELLED

99 HH nonresonant and self-coupling at ATLAS+CMS

Speaker: Laura Pereira Sanchez (Stockholm University (SE))

LauraPereira_HH_LHCP.pdf

Recording

100 HH production in a global EFT Higgs fit

Speaker: Ramona Groeber (Università di Padova and INFN, Sezione di Padova)

LHCP21_ramona.pdf

Recording

Joint sessions: Heavy ions and QCD

LHC_JointHiggsTop.pdf

101 Nuclear parton distribution functions

Speaker: Cynthia Keppel (Jefferson Lab)

~$LHCP2021_Keppel.pptx

102 New results on the modification of jet structure in Heavy Ion collisions

Speaker: Helena Santos (LIP - Lisbon)

LHCP2021_HSantos.pdf

Recording

103 Nuclear shadowing and heavy ion UPCs at the LHC

Speaker: Vadim Guzey (NRC Kurchatov Institute PNPI (RU))

guzey_LHCP_2021.pdf

Recording

104 New measurements on Photon-Photon interactions

Speaker: Ruchi Chudasama (Tata Inst. of Fundamental Research (IN))

LHCP_photon_photon_ruchi.pdf

Recording

105 New measurements on diffractive vector mesons

Speaker: Simone Ragoni (University of Birmingham (GB))

LHCP2021.pdf

Recording

Joint sessions: Upgrades and performance

Conveners: Christian Ohm (KTH Royal Institute of Technology (SE)), Nicole Skidmore (University of Bonn (DE)), Nora Emilia Pettersson (CERN), Saptaparna Bhattacharya (Northwestern University (US))

LHC_JointHiggsTop.pdf

106 Improvements for reconstruction of physics objects with HL-LHC detector upgrades for ATLAS and CMS

Speaker: Adriano Di Florio (Universita e INFN, Bari (IT))

LHCP_Reco_Adriano.pdf

Recording

107 Use of hardware acceleration for online event reconstruction for Run 3 and later

Speaker: Marten Ole Schmidt (Ruprecht Karls Universitaet Heidelberg (DE))

HardwareAccelerationOnlineReco_final.pdf

Recording

108 Status and prospects for technical solutions for real-time analysis for Run-3 and later

Speaker: Miguel Ramos Pernas (University of Warwick (GB))

Miguel_Ramos_Pernas_LHCP2021.pdf

Recording

109 Particle identification and tracking with timing detectors in ALICE and LHCb in Run 5

Speaker: Stefania Bufalino (Politecnico di Torino (IT))

LHCP2021_Bufalino.pdf

Recording

110 HL-LHC Computing Challenges - how can the physics performance be maintained?

Speaker: Vincent Pascuzzi (Lawrence Berkeley National Lab. (US))

Google Slides

Recording

15:45 Coffee break

Plenary II: Beyond the Standard Model - TeV scale

Conveners: Andrea Wulzer (CERN and EPFL), Marc Besancon (cea-saclay/dapnia/spp)

111 Searches for supersymmetry

Speaker: Elodie Deborah Resseguie (Lawrence Berkeley National Lab. (US))

LHCP2021_SUSY_er.pdf

Recording

112 Searches for exotica

Speaker: Halil Saka (University of Cyprus (CY))

ExoticSearches_LHCP_HS.pdf

Recording

113 New ideas for TeV-scale model building

Speaker: Veronica Sanz Gonzalez (University of Sussex (GB))

LHCP21.pdf

Recording

114 SMEFT and searches for new physics

Speaker: Alex Pomarol (Universitat Autonoma de Barcelona & IFAE)

LHCP 21.pdf

Recording

115 Dark Matter: overview of collider-based and direct / indirect searches

Speaker: Deborah Pinna (University of Wisconsin Madison (US))

DarkMatter_LHC_LHCP_DP.pdf

Recording

Wednesday 9 June

Plenary III: Electroweak Physics

Conveners: Andrew Pilkington (University Of Manchester), Radja Boughezal (Argonne National Laboratory)

116 Low energy probes of the electroweak sector

Speaker: Michael Ramsey-Musolf (Shanghai Jiao Tong University)

MJRM LHCP EW 21.pdf

Recording

117 EWK precision measurements

Speaker: Ilya Gorbunov (Joint Institute for Nuclear Research (RU))

GorbunovLHCP21.pdf

Recording

118 Multiboson measurements

Speaker: Antonio Giannini (Universita e sezione INFN di Napoli (IT))

LHCPConference_AGiannini_Jun21.pdf

Recording

119 VBF and VBS measurements

Speaker: Roberto Covarelli (University/INFN Torino (IT))

LHCP21_vbs.pdf

Recording

13:30 Coffee break

Joint sessions: Flavour physics and QCD

LHC_JointHiggsTop.pdf

120 Heavy-flavour hadron production

Speaker: Mattia Faggin (Universita e INFN, Padova (IT))

mfaggin_LHCp2021_HFprod_final.pdf

Recording

121 Heavy Flavour production in MC

Speaker: Stefan Hoeche (Fermilab)

paris_21-06.pdf

Recording

122 Experimental measurement of Heavy Flavours and jets

Speaker: Meena Meena (Panjab University (IN))

Meena_LHCP2021_heavy_flavor_jets.pdf

Recording

123 Theoretical view on Heavy Flavours and jets

Speaker: Maria Ubiali (University of Cambridge)

LHCp_Ubiali.pdf

Recording

124 New measurements in the quarkonia sector

Speaker: Valeriia Zhovkovska (Université Paris-Saclay (FR))

20210609_LHCP_Quarkonium_Zhovkovska.pdf

Recording

Joint sessions: Higgs and top physics

Conveners: Maria Moreno Llacer (Univ. of Valencia and CSIC (ES)), Meng Xiao (ZJU - Zhejiang University (CN))

LHC_JointHiggsTop.pdf

125 ttX calculations and modeling

Speaker: Andrea Ferroglia (New York City College of Technology CUNY)

LHCP_21_Ferroglia.pdf

Recording

126 ttX results from ATLAS+CMS

Speaker: Peter Johannes Falke (University of Bonn (DE))

Recording

ttX_at_ATLAS_and_CMS_PeterFalke.pdf

127 ttH results from ATLAS+CMS

Speaker: Dr Djamel Eddine Boumediene (Université Clermont Auvergne (FR))

Recording

ttH-ATLAS-CMS-LHCP2021.pdf

128 Determination of kappatop from ttbar, 4top, ...

Speaker: Emanuele Usai (Brown University (US))

LHCP21Usai 3.pdf

Recording

Joint sessions: Joint BSM session

Conveners: Niki Saoulidou (National and Kapodistrian University of Athens (GR)), Seema Sharma (Indian Institute of Science Education and Research (IN))

LHC_JointHiggsTop.pdf

129 Dark Matter at colliders: theory

Speaker: Victor Martin-Lozano (DESY)

DM-theory-VMLozano.pdf

Recording

130 Search for high mass mediators in ATLAS and CMS

Speaker: Claudio Quaranta (Sapienza Universita e INFN, Roma I (IT))

Recording

Search for high mass mediators in ATLAS and CMS.pdf

131 Search for low mass mediators in ATLAS and CMS

Speaker: Silvio Donato (Universita & INFN Pisa (IT))

lowMassResonance_Donato.pdf

Recording

132 Mono-jet, Mono-V searches in ATLAS and CMS

Speaker: Varun Sharma (University of Wisconsin Madison (US))

2021-06-LHCP2021.pdf

Recording

133 Mono-Higgs, Mono-top searches in ATLAS and CMS

Speaker: Mariana Toscani (Universidad de Buenos Aires (AR))

mono-H_mono-top_in_BSM_searches_v5.pdf

Recording

Outreach and diversity: Session 1

Conveners: Benoit Blossier (CNRS/Laboratoire de Physique Théorique d'Orsay), Federica Baldassari (CERN), Federico Leo Redi (EPFL - Ecole Polytechnique Federale Lausanne (CH)), Federico Ronchetti (INFN e Laboratori Nazionali di Frascati (IT)), Dr Kate Shaw (University of Sussex (GB))

134 LHC and outreach

Speaker: Violaine Bellee (Universitaet Zuerich (CH))

2021_06_09_LHCPOutreach_Bellee.pdf

Recording

135 LHC and diversity

Speaker: Adriana Telesca (CERN)

20210609_AT_LHCP2021_v12.pdf

Recording

136 LHC experiments and their Open Data

Speaker: Edgar Fernando Carrera Jarrin (Universidad San Francisco de Quito (EC))

LHCExpOpenData_ECarrera_LHCP2021.pdf

Recording

137 The IPPOG Resource Database: Making particle physics outreach & education available worldwide

Speaker: Barbora Bruant Gulejova (Universitaet Bern (CH))

IPPOG_RDB_LHCP_2021_BBG_final.pdf

IPPOG_RDB_LHCP_2021_BBG_final.pptx

Recording

138 A beamline for schools

Speaker: Margherita Boselli (CERN)

Beamline_for_Schools.pdf

Recording

Tools: Experimental tools

Conveners: Andy Buckley (University of Glasgow (GB)), Loukas Gouskos (CERN), Philip Ilten (University of Cincinnati (US)), Sandro Christian Wenzel (CERN), Stefano Carrazza (CERN)

139 Advances in detector simulation tools

Speaker: Samuel Louis Bein (Hamburg University (DE))

LHCp2021_LhcSimulationRandDb.pdf

Recording

140 Deep learning approaches in analysis

Speaker: Lukas Alexander Heinrich (CERN)

LHCP_DeepLearning.pdf

Recording

141 GPUs in trigger and reconstruction algorithms

Speaker: Thomas Boettcher (University of Cincinnati (US))

boettcher_LHCP_9June2021_v5.pdf

Recording

142 Advances in experimental analysis frameworks

Speaker: Jan Fiete Grosse-Oetringhaus (CERN)

Recording

v8.pdf

143 Discussion

Upgrades: Detectors at HL-LHC

Conveners: Christian Ohm (KTH Royal Institute of Technology (SE)), LianTao Wang (University of Chicago), Magnus Mager (CERN), Saptaparna Bhattacharya (Northwestern University (US)), Silvia Borghi (University of Manchester (GB))

LHCPInstructions.pdf

144 Novel detector concepts for ALICE for Run 4 and beyond

Speaker: Giacomo Contin (Universita e INFN Trieste (IT))

LHCP_ALICE_Novel_Detectors_Contin.pdf

Recording

145 Status and progress on the ATLAS Phase-II detector upgrades

Speaker: Oleg Solovyanov (Institute for High Energy Physics of NRC Kurchatov Institute (RU))

Recording

Solovyanov_LHCP2021.pdf

146 Status and progress on the CMS Phase-II detector upgrades

Speaker: Nadja Strobbe (University of Minnesota (US))

LHCP2021_CMS_PhaseII_Strobbe.pdf

Recording

147 Status and progress for LHCb Upgrade-II detector

Speaker: Silvia Gambetta (The University of Edinburgh (GB))

LHCb_UpgradeII_LHCP_sg.pdf

Recording

148 Results from commissioning and/or prototypes for new small (HL-)LHC experiments

Speaker: Friedemann Neuhaus (Johannes Gutenberg Universitaet Mainz (DE))

fneuhaus_lhcp.pdf

Recording

15:15 Coffee break

BSM - Feebly Interacting Particles: Unconventional signatures

Conveners: Emma Torro Pastor (Univ. of Valencia and CSIC (ES)), José Francisco Zurita, Niki Saoulidou (National and Kapodistrian University of Athens (GR)), Vasiliki Mitsou (Univ. of Valencia and CSIC (ES)), Xabier Cid Vidal (Instituto Galego de Física de Altas Enerxías)

149 Theoretical overview of Dark Showers

Speaker: Elias Bernreuther (RWTH Aachen University)

lhcp_darkshowers.pdf

Recording

150 Searches for Dark Showers at the LHC

Speaker: Aran Garcia-Bellido (University of Rochester (US))

AGB_DarkShowers_LHCP21.pdf

Recording

151 Searches for Disappearing Tracks, HSCPs and Stopped Particles at the LHC

Speaker: Emma Sian Kuwertz (University of Bristol)

FIP_SPDT_LHCP2021.pdf

Recording

152 Searches for Anomalous Ionizing Particles, SIMPs, and Monopoles at the LHC

Speaker: Claudia Wulz (Austrian Academy of Sciences (AT))

Wulz_LHCP_June2021.pdf

Wulz_LHCP_June2021.pptx

153 Status of MoEDAL and milliQan experiments

Speaker: Michael Staelens

LHCP2021 Presentation - MoEDAL & milliQan v3 .pdf

Recording

154 Round table discussion

Flavour physics: Session 2

Conveners: Diego Guadagnoli (LAPTh Annecy), Dmytro Kovalskyi (Massachusetts Inst. of Technology (US)), Michel De Cian (EPFL - Ecole Polytechnique Federale Lausanne (CH)), Sarah Porteboeuf (Université Clermont Auvergne (FR)), Semen Turchikhin (Joint Institute for Nuclear Research (RU))

155 CP violation in charm with the LHCb experiment

Speaker: Serena Maccolini (Universita e INFN, Bologna (IT))

Recording

SMaccolini_LHCP21_CPV_in_charm.pdf

156 CP violation in beauty with the LHCb experiment

Speaker: Alessandro Bertolin (Universita e INFN, Padova (IT))

bertolinLHCP2021.pdf

bertolinLHCP2021.pptx

Recording

157 CP violation with the ATLAS and CMS experiments

Speaker: Adam Edward Barton (Lancaster University (GB))

CMSATLAS_CPV_results.pdf

Recording

158 Theory Overview of CP violation in the Charm sector

Speaker: Yuval Grossman (Cornell)

LHCp-2021.pdf

Recording

159 CKM Metrology theory

Speaker: Stefan Schacht (University of Manchester)

lhcp-2021-schacht.pdf

Recording

Heavy ions: Collectivity of soft and heavy flavour

Conveners: Alexander Rothkopf (University of Stavanger), Hengne Li (South China Normal University (CN)), Maximiliano Puccio (CERN), Qipeng Hu (Lawrence Livermore Nat. Laboratory (US)), Wei Li (Rice University (US))

160 Origin of collectivity in QCD systems

Speaker: Giuliano Giacalone (Université Paris-Saclay)

Recording

talk.pdf

161 Collectivity of soft probes in small systems

Speaker: Tomasz Bold (AGH Univ. of Science and Technology, Krakow (PL))

2021-06-lhcp-soft-collectivity.pdf

Recording

162 Heavy flavor collectivity in small systems

Speaker: Dr Georgios Krintiras (The University of Kansas (US))

Flow_small_systems.pdf

Recording

163 Collectivity of soft probes in heavy ion collisions

Speaker: Vytautas Vislavicius (University of Copenhagen (DK))

Recording

Vislavicius_LHCP21.pdf

164 Heavy flavor collectivity in heavy ion collisions

Speaker: Fabrizio Grosa (CERN)

LHCP2021_HFcollectivity_fgrosa.pdf

Recording

165 Collectivity in UPC

Speaker: Peter Alan Steinberg (Brookhaven National Laboratory (US))

Recording

Steinberg_LHCP2021_v1.pdf

Joint sessions: EFT interpretations

LHC_JointHiggsTop.pdf

166 Theory aspects in global analyses

Speaker: Eleni Vryonidou (University of Manchester (GB))

LHCP2021.pdf

Recording

167 EFT computations

Speaker: Ilaria Brivio (University of Heidelberg)

Recording

slides_LHCP_2021.pdf

168 Experimental EFT results

Speaker: Nicolas Morange (Université Paris-Saclay (FR))

EFT_ATLAS-CMS.pdf

Recording

169 Open questions from the LHC EFT WG

Speaker: Admir Greljo (Universitaet Bern (CH))

LHCP-EFT.pdf

Recording

170 Discussion

Recording

Outreach and diversity: Session 2

Conveners: Benoit Blossier (CNRS/Laboratoire de Physique Théorique d'Orsay), Federica Baldassari (CERN), Federico Leo Redi (EPFL - Ecole Polytechnique Federale Lausanne (CH)), Federico Ronchetti (INFN e Laboratori Nazionali di Frascati (IT)), Kate Shaw (University of Sussex (GB))

171 Arts and science in Italy: from high-schools to CERN

Speaker: Dr Pierluigi Paolucci (Universita e INFN of Napoli (IT))

LHCP 2021 Pierluigi Paolucci.pptx

Recording

172 EEE (Extreme Energy Events)

Speaker: Dr Silvia Pisano (INFN e Laboratori Nazionali di Frascati (IT))

outreach_EEE_LHCP21.pdf

Recording

173 Astronomy for all: a reality even for people with disabilities

Speaker: Ludovic Petitdemange

Astronomy for all - LP.pdf

Recording

174 ResearchAbility: do we really need a more inclusive environment in research?

Speaker: Gian Maria Greco (Marie Curie Alumni Association & University of Warsaw)

GMGreco_MCAA_RA_LHCP2021.pdf

Recording

Tools: Other tools

Conveners: Andy Buckley (University of Glasgow (GB)), Loukas Gouskos (CERN), Philip Ilten (University of Cincinnati (US)), Sandro Christian Wenzel (CERN), Stefano Carrazza (CERN)

175 Advances in software management tools

Speaker: Jakob Blomer (CERN)

software-lhcp21.pdf

176 ML and advances in Data Quality Monitoring

Speaker: Suzanne Klaver (Nikhef National institute for subatomic physics (NL))

LHCP_SuzanneKlaver_v2.pdf

177 Quantum Information Science in HEP

Speaker: Dr Jean-Roch Vlimant (California Institute of Technology (US))

vlimant_LHCP-QIS_June21.pdf

178 Advances in Analysis tools/ecosystem

Speaker: Oksana Shadura (University of Nebraska Lincoln (US))

Advances in Analysis tools/ecosystem

LHCP_AS.pdf

179 Discussion

Upgrades: Future colliders

Conveners: Christian Ohm (KTH Royal Institute of Technology (SE)), LianTao Wang (University of Chicago), Magnus Mager (CERN), Saptaparna Bhattacharya (Northwestern University (US)), Silvia Borghi (University of Manchester (GB))

LHCPInstructions.pdf

180 Prospects for future colliders and advanced accelerator technologies

Speaker: Akira Yamamoto (High Energy Accelerator Research Organization (JP))

LHCP2021-ay-210609a.pdf

Recording

181 Requirements, emerging technologies, and challenges for detectors at future accelerators

Speaker: Didier Claude Contardo (Centre National de la Recherche Scientifique (FR))

LHCP_DC_09062021.pdf

LHCP_DC_09062021.pptx

Recording

182 The BSM Physics Case for Future Hadron Colliders

Speaker: Matthew Reece (Harvard University)

Recording

Reece_LHCP_FutureColliders_2021.pdf

183 Towards a multi-TeV Muon Collider

Speaker: Nadia Pastrone (Universita e INFN Torino (IT))

LHCP_NPastrone_MuonCollider_9jun21.pdf

184 Physics at future lepton colliders

Speaker: Matthew Philip Mccullough (CERN)

LHCP.pdf

17:00 Coffee break

Plenary IV: Beyond the Standard Model - feebly interacting particles

Conveners: Laura Patrizii (Universita e INFN, Bologna (IT)), Wolfgang Adam (HEPHY-Vienna)

185 FIPs: phenomenology overview and new ideas

Speaker: Gilad Perez (Weizmann)

Gilad_Perez_LHCP21.pdf

Recording

186 Searching for Charged FIPs and HIPS (Monopoles, Dyons, etc) at the LHC and Beyond

Speaker: James Pinfold (University of Alberta (CA))

FIP abd HIPs LHCP 2021.pdf

Recording

187 Searching for neutral FIPs at LHC and beyond

Speaker: Lawrence Lee Jr (Harvard University (US))

060921_LLee_NeutralFIPs.pdf

Recording

188 Cosmology constraints on Dark Sector models for colliders

Speaker: GOUDELIS Andreas (LPC - Clermont Ferrand)

AndreasLHCP2021.pdf

Recording

Thursday 10 June

Plenary V: Flavour Physics

Conveners: Marie-Helene Schune (Université Paris-Saclay (FR)), Sebastien Descotes-Genon (Laboratoire de Physique Théorique d'Orsay)

189 Heavy flavour - theory

Speaker: Andreas Crivellin (Universitaet Zuerich (CH))

LHCP2021.pdf

LHCP2021.pptx

Recording

190 Heavy flavour results from non-LHC experiments

Speaker: Justine Serrano (Aix Marseille Univ, CNRS/IN2P3, CPPM, Marseille, France)

LHCP2021_justine.pdf

Recording

191 B-hadrons: CPV and semileptonic decays

Speaker: Basem Khanji (Technische Universitaet Dortmund (DE))

LHCP_2021_BKhanji.pdf

Recording

192 Rare decays

Speaker: Alessio Boletti (LIP, Lisboa (PT))

RareDecays_LHCP2021_Boletti.pdf

Recording

193 Heavy flavour production and spectroscopy

Speaker: Jibo He (University of Chinese Academy of Sciences (CN))

20210610_HFPS.pdf

Recording

14:00 Coffee break

TeV-scale BSM: Third generation and flavour

Conveners: Carl Gwilliam (University of Liverpool (GB)), Seema Sharma (Indian Institute of Science Education and Research (IN)), Yael Shadmi (Technion)

194 ATLAS + CMS searches for third generation SUSY particles

Speaker: Daniel Spitzbart (Boston University (US))

LHCP_2021_3rd_gen.pdf

Recording

195 ATLAS + CMS searches for leptoquarks

Speaker: Edson Carquin Lopez (Federico Santa Maria Technical University (CL))

ECarquinTalkFinal.pdf

Recording

196 ATLAS + CMS searches for vector-like quarks

Speaker: Timothy Robert Andeen (University of Texas at Austin (US))

AndeenLHCP_vFinal.pdf

Recording

197 Flavour tagging for enhancing sensitivity to new physics

Speaker: Yotam Soreq (Technion- Israel Institute of Technology (IL))

2021_06_LHCP_2021.pdf

Recording

198 Discussion

Electroweak physics: Precision

Conveners: Davide Pagani (Deutsches Elektronen-Synchrotron (DE)), Hang Yin (Central China Normal University CCNU (CN)), Joany Manjarres (Technische Universitaet Dresden (DE)), Pietro Vischia (Universite Catholique de Louvain (UCL) (BE))

199 Precision measurements, W mass, sinθw (theory)

Speaker: Ayres Freitas (University of Pittsburgh)

lhcp21_freitas.pdf

Recording

200 W mass and angular coefficients measurements ATLAS-CMS-LHCb

Speaker: Martina Pili (University of Oxford (GB))

Pili_LHCP_V4.pdf

Recording

201 Rare decay search ATLAS+CMS

Speaker: Riccardo Salvatico (The University of Kansas (US))

RareDecays_LHCP.pdf

Recording

202 Discussion

Recording

Flavour physics: Session 3

Conveners: Diego Guadagnoli (LAPTh Annecy), Dmytro Kovalskyi (Massachusetts Inst. of Technology (US)), Michel De Cian (EPFL - Ecole Polytechnique Federale Lausanne (CH)), Sarah Porteboeuf (Université Clermont Auvergne (FR)), Semen Turchikhin (Joint Institute for Nuclear Research (RU))

203 Classical spectroscopy

Speaker: Valentina Mariani (Universita e INFN, Perugia (IT))

Flavours_LHCP .pdf

Recording

204 Tetra- and pentaquark "spectroscopy"

Speaker: Elisabetta Spadaro Norella (Università degli Studi e INFN Milano (IT))

LHCP21_Spadaro.pdf

Recording

205 Recent Belle2 results and projections

Speaker: Frank Meier (Duke University)

LHCP_FlavorPhysicsAtBelle2.pdf

Recording

206 [CANCELLED] LQCD calculations for flavour phenomenology: highlights and prospects

Speaker: Antoine Gérardin (U. Aix-Marseille)

207 Round Table

Recording

Higgs physics: Session 3

Conveners: Giuliano Panico (University of Florence and INFN Florence), Kerstin Tackmann (Deutsches Elektronen-Synchrotron (DE)), Meng Xiao (ZJU - Zhejiang University (CN))

208 Fiducial and differential measurements at ATLAS+CMS

Speaker: Roberto Seidita (Universita e INFN, Firenze (IT))

Higgs_fiducial_and_differential_measurements_at_ATLAS_and_CMS_final.pdf

Recording

209 Precision computations for Higgs production

Speaker: Johannes Michel (MIT CTP)

LHCP_Johannes_Michel_2021_06_10.pdf

Recording

210 High-pT Higgs production

Speaker: Raoul Horst Rontsch (CERN)

LHCP2021_roentsch.pdf

Recording

211 Discussion

LHCP2021_HiggsDiscussion.pdf

Recording

Detector performance: Session 2

Conveners: Francesco Prino (Universita e INFN Torino (IT)), Nicole Skidmore (University of Bonn (DE)), Nora Emilia Pettersson (CERN), Phat Srimanobhas (Chulalongkorn University (TH))

212 Tracking in ATLAS and CMS

Speaker: Mia Tosi (Università degli Studi di Padova & INFN)

210607_LHCP2021_miatosi_tracking.pdf

Recording

213 Flavour-tagging / Jet / Met performance in ATLAS and CMS

Speaker: Jonathan Bossio (CERN)

JonaBossio_LHCP21.pdf

Recording

214 ALICE: new inner tracker commissioning and impact on vertexing in Run 3

Speaker: Ivan Ravasenga (Nikhef National institute for subatomic physics (NL))

LHC2021_iravasen_v5.pdf

Recording

215 LHCb: tracking and flavour-tagging and PID

Speaker: Vitalii Lisovskyi (Technische Universitaet Dortmund (DE))

LHCP2021_latest.pdf

Recording

216 Round table discussion

Recording

QCD: Precision Measurements

Conveners: Ben Nachman (Lawrence Berkeley National Lab. (US)), Frank Petriello (Northwestern University and Argonne National Lab), Gabor Veres (Eotvos Lorand University (HU)), Joe Osborn (Oak Ridge National Laboratory), Laura Brittany Havener (Yale University (US))

217 Recent progress on high order calculations and matching to parton showers

Speaker: Emanuele Re (Unite Reseaux du CNRS (FR))

2021_06_09.pdf

Recording

218 Precision QCD Measurements from CMS

Speaker: Salim Cerci (Adiyaman University (TR) - Istanbul University (TR))

LHCP2021_Salim_Cerci.pdf

Recording

219 Precision QCD Measurements from ATLAS

Speaker: Tibor Zenis (Comenius University (SK))

Recording

Zenis_Precision_QCD_Measurements_from_ATLAS.pdf

220 Precision QCD Measurements from LHCb

Speaker: Marcin Kucharczyk (Polish Academy of Sciences (PL))

LHCP_2021_Kucharczyk_v2.pdf

Recording

221 Precision QCD Measurements from ALICE

Speaker: Dimitar Lubomirov Mihaylov (Technische Universitaet Muenchen (DE))

Mihaylov_LHCP2021.pdf

Recording

Top physics: Top mass and properties

Conveners: Gauthier Durieux (CERN), Jose Enrique Palencia Cortezon (Universidad de Oviedo (ES)), Maria Moreno Llacer (Univ. of Valencia and CSIC (ES)), Stephen Farry (University of Liverpool (GB))

Top@LHCP2021.pdf

222 Top Properties and Asymmetry measurements at the LHC

Speaker: Nils Faltermann (KIT - Karlsruhe Institute of Technology (DE))

21-06-10_LHCP.pdf

Recording

223 Top Measurement Highlights at CMS

Speaker: Mintu Kumar (Tata Inst. of Fundamental Research (IN))

Recording

Single_top_highlights_LHCP Talk_by_Mintu_kumar.pdf

Single_top_highlights_LHCP Talk_by_Mintu_kumar.pptx

224 Top Measurement Highlights at ATLAS

Speaker: Stefan Richter (DESY)

Recording

StefanRichter_LHCP2021.pdf

225 Theory status of top properties

Speaker: Alexander Mitov (University of Cambridge (GB))

AlexanderMitov-LHCP-2021.pdf

AlexanderMitov-LHCP-2021.pptx

226 General Discussion

Recording

15:45 Coffee break

Plenary VI: Higgs Physics

Conveners: Jeonghyeon Song (Konkuk University), Rosy Nikolaidou (Université Paris-Saclay (FR))

227 Probing the SMEFT using the electroweak sector

Speaker: Shankha Banerjee (CERN)

LHCP_Banerjee.pdf

Recording

228 Higgs physics - experimental talk

Speaker: Pierluigi Bortignon (INFN Padova (IT) and Universita di Cagliari)

202106-lhcp-higgs-experimential-bortignon-final.pdf

Recording

229 Rare and BSM Higgs decays

Speaker: Imma Riu (IFAE Barcelona (ES))

Rare-BSM-HiggsDecays-LHCP-2021.pdf

Recording

230 Precision calculations of Higgs boson properties

Speaker: Bernhard Mistlberger (SLAC National Accelerator Laboratory (US))

Mistlberger_LHCP21.pdf

Recording

231 Constraints on BSM from the Higgs sector

Speaker: Jorge de Blas (Universidad de Granada (ES))

BSM_Higgs_deBlas_LHCP21.pdf

Recording

Poster Session

232 $\rm \Omega_{c}^{0}$ production cross section in pp collisions at $\sqrt{s}=$ 13 TeV with ALICE

Recent measurements of charm-baryon production at midrapidity by the ALICE collaboration in pp collisions show baryon-over-meson ratios significantly higher than those in $\rm e^+e^-$ collisions for different charm-hadron species. The charmed baryon-to-meson and charmed baryon-to-baryon ratios provide unique information on hadronisation mechanisms. In this poster, the first measurement of production cross section of $\rm \Omega_{c}^{0}$ via the hadronic decay channel $\rm \Omega_{c}^{0} \rightarrow \pi^{+} \Omega^{-}$ (and its charge conjugate) in $2

Speaker: Jianhui Zhu (Central China Normal University CCNU (CN))

20210610_LHCP_Jianhui_v6.pdf

Zoom meeting room

233 $\rm{\Lambda^{+}_{c}}$ cross section in pp and p--Pb collisions down to $p_{\rm T}$ = 0 at $\sqrt{s_{\rm NN}}$ = 5.02 TeV measured with ALICE

The production cross sections of open heavy-flavour hadrons are typically described within the factorisation approach as the convolution of the parton distribution functions of the incoming protons, the perturbative QCD partonic cross section, and the fragmentation functions. These last are typically parametrised from measurements in ${\rm e^+e^-}$ collisions. Measurements of charm-baryon production are crucial to study the charm quark hadronisation in pp and p--Pb collisions and its difference with respect to ${\rm e^+e^-}$ collisions. Furthermore, measurements of charm-baryon production in p--Pb collisions provide important information about Cold Nuclear Matter (CNM) effects quantified in the nuclear modification factor $R_{\rm pPb}$. Measurements in p--Pb collisions also help us to understand how the possible presence of collective effects could modify the production of heavy-flavour hadrons and to find similarities among pp, p--Pb and Pb--Pb systems.
In this poster, the latest measurements of $\Lambda^+_{\rm c}$ performed with the ALICE detector at midrapidity in pp, and the new measurement performed down to $p_{\rm T}=0$ in p--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV are presented. This allows us to show the first ALICE measurement of $\Lambda^+_{\rm c}/{\rm D^0}$ and $\Lambda^+_{\rm c}$ $R_{\rm pPb}$ down to $p_{\rm T}$ = 0 in p--Pb collisions. The $\Lambda^+_{\rm c}/{\rm D^0}$ ratio at midrapidity in small systems is significantly higher than the one in ${\rm e^+e^-}$ collisions, suggesting that the fragmentation of charm is not universal across different collision systems. Results are compared with theoretical calculations.

Speaker: Annalena Sophie Kalteyer (GSI - Helmholtzzentrum fur Schwerionenforschung GmbH (DE))

LcTopKs0_lowpT_Kalteyer_LHCP2021.pdf

Zoom meeting room

234 A High-Granularity Timing Detector for the ATLAS Phase-II upgrade

The increase of the particle flux (pile-up) at the HL-LHC with instantaneous luminosities up to
L ~ 7.5 × 10$^{34}$ cm$^{-2}$s$^{-1}$ will have a severe impact on the ATLAS detector reconstruction and trigger performance. The end-cap and forward region where the liquid Argon calorimeter has coarser granularity and the inner tracker has poorer momentum resolution will be particularly affected. A High Granularity Timing Detector (HGTD) will be installed in front of the LAr end-cap calorimeters for pile-up mitigation and luminosity measurement.
The HGTD is a novel detector introduced to augment the new all-silicon Inner Tracker in the pseudo-rapidity range from 2.4 to 4.0, adding the capability to measure charged-particle trajectories in time as well as space. Two silicon-sensor double-sided layers will provide precision timing information for minimum-ionising particles with a resolution as good as 30 ps per track in order to assign each particle to the correct vertex. Readout cells have a size of 1.3 mm × 1.3 mm, leading to a highly granular detector with 3.7 million channels. Low Gain Avalanche Detectors (LGAD) technology has been chosen as it provides enough gain to reach the large signal over noise ratio needed.
The requirements and overall specifications of the HGTD will be presented as well as the technical design and the project status. The on-going R&D effort carried out to study the sensors, the readout ASIC, and the other components, supported by laboratory and test beam results, will also be presented.

Speaker: Asmaa Aboulhorma (Universite Mohammed V (MA))

LHCP-poster.pdf

LHCP-Slides.pdf

Zoom meeting room

235 A Search for Lepton-Flavour-Violating Z->etau and Z->mutau Decays with the ATLAS Experiment

In the Standard Model (SM), lepton flavour is conserved in all interactions.
Hence, any observation of lepton flavour violation (LFV) would be an
unambiguous sign of physics beyond the SM (BSM), and LFV processes are
predicted by numerous BSM models.
One way to search for LFV is in the decay of gauge bosons.
In the search presented here, the decay of the Z boson to an electron-tau or
muon-tau pair is investigated using the full Run 2 pp collision data set at
sqrt(s) of 13TeV recorded by the ATLAS experiment at the LHC.
The analysis exploits tau decays into hadrons and - for the first time in this
channel in ATLAS - into leptons.
A key ingredient of the search is the usage of a neural net to differentiate
between signal and background events in order to make optimum use of the data.
Combined with about 8 billion Z decays recorded by ATLAS in Run 2 of the LHC,
the strongest constraints to date are set with Br(Z->etau)<5.0e-6 and
Br(Z->mutau)<6.5e-6 at 95% confidence level
- finally superseding the limits set by the LEP experiments more than two
decades ago.

Speaker: Ann-Kathrin Perrevoort (Nikhef National institute for subatomic physics (NL))

LHCP_Perrevoort_2021.pdf

Poster video explanation

Zoom meeting room

236 AFP Performance in the Low Pile-up Runs

Since 2016 ATLAS detector is equipped with new devices - ATLAS Forward Proton (AFP) detectors. AFP aims to measure protons scattered at very small angles, which are a natural signature of so-called diffractive events. Measurement of properties of diffractive events usually require low pile-up data-taking conditions. AFP performance in such special, low pile-up runs, including evaluation of detector efficiency, will be presented.

Speaker: Maciej Piotr Lewicki (Polish Academy of Sciences (PL))

LHCP2021.pdf

Zoom meeting room

237 Analysis of b-jets production in p–Pb and pp collisions at √sNN = 5.02 TeV with ALICE

Production of beauty quarks takes place mostly in initial hard scattering processes and can be calculated using perturbative quantum chromodynamics (pQCD). Thanks to excellent particle tracking capabilities, the ALICE experiment at the LHC is able to reconstruct beauty-hadron decay vertices, displaced hundreds of micrometers from the primary interaction vertex. The poster will present inclusive pT spectra of b jets measured in p–Pb and pp collisions at √sNN = 5.02 TeV, the corresponding nuclear modification factor, and the fraction of b jets among inclusive jets. The production cross-section of b jets was measured down to 10 GeV/c which is lower than in previous measurements of b jets done at the LHC. Low pT b-jets are expected to be more sensitive to cold nuclear matter effects in p–Pb collisions. They are an important reference for future Pb–Pb measurements, where their production provides information on color and parton mass dependence of parton energy loss.

Speaker: Artem Isakov (Czech Academy of Sciences (CZ))

aisakov_alice_bjets.pdf

Video

Zoom meeting room

238 Angular correlations of heavy-flavour decay electrons and charged particles in pp and p-Pb collisions $\sqrt{s_{\rm NN}}=$ 5.02 TeV with ALICE at LHC.

Heavy quarks (charm, beauty), due to the large masses, mainly originate via hard partonic scattering processes in high-energy hadronic collisions. They evolve as parton showers and hadronize as back-to-back jet events.

Two particles azimuthal angular correlations triggered by electrons from heavy-flavour hadron decays can be used for heavy-flavor jet studies. Such correlation distributions contains a near-side peak around $\Delta\varphi = 0$ formed by particles associated with a high-$p_{\rm T}$ trigger particle, and an away-side peak around $\Delta\varphi = \pi$. By changing the momentum scales of the trigger and associated particles one can study the heavy-flavour jet structure. In pp collisions, heavy-flavour correlations can be used to study the production and fragmentation of heavy-quarks. In p-Pb collisions, heavy-flavour correlations can be used to test cold nuclear matter and gluon saturation effects.

In this poster, we present the current status and results of the ALICE measurement of azimuthal angular correlations of high-$p_{\rm T}$ heavy-flavour decay electrons with charged particles in pp and p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV from the LHC Run 2 data. The results from pp and p-Pb collisions will be compared with each other to investigate any modification due to cold nuclear matter effect.

Speaker: Ravindra Singh (Indian Institute of Technology Indore (IN))

Angular correlations of heavy-flavour decay electrons and charged particles in pp collision at √s = 5.02 TeV with ALICE at LHC(1).pdf

Zoom meeting room

239 Apparent modification of the jet-like yield in high multiplicity proton-proton collisions

In this work we present the production of charged particles associated with high-$p_{\rm T}$ trigger particles ($8<\textit{p}_{\rm T}^{\rm trig.}<15$ GeV/$c$) at midrapidity in proton-proton collisions at $\sqrt{s}=5.02$,TeV simulated with the PYTHIA 8 Monte Carlo model [1]. The study is performed as a function of the relative transverse activity classifier, $R_{\rm T}$, which is the relative charged-particle multiplicity in the transverse region ($\pi/3< \phi^{\rm trig.}-\phi^{\rm assoc.}|<2\pi/3$) of the di-hadron correlations, and it is sensitive to the Multi-Parton Interactions. The evolution of the yield of associated particles on both the towards and the away regions ($3\leq p_{\rm T}^{\rm assoc.}< 8$ GeV/$c$) as a function of $R_{\rm T}$ is investigated. We propose a strategy which allows for the modelling and subtraction of the Underlying Event (UE) contribution from the towards and the away regions in challenging environments like those characterised by large $R_{\rm T}$. We found that the signal in the away region becomes broader with increasing $R_{\rm T}$. Contrarily, the yield increases with $R_{\rm T}$ in the towards region. This effect is reminiscent of that seen in heavy-ion collisions, where an enhancement of the yield in the towards region for 0-5% central Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}=2.76$,TeV was reported. To further understand the role of the UE and additional jet activity, the transverse region is divided into two one-sided sectors, "trans-max" and "trans-min" selected in each event according to which region has larger or smaller charged particle multiplicity. Based on this selection criterium, the observables are studied as a function of $R_{\rm T}^{\rm max}$ and $R_{\rm T}^{\rm min}$, respectively. Results for pp collisions simulated with PYTHIA 8.244 and Herwing 7.2 will be shown.

[1] J.Phys.G 48 (2020) 1, 015007

Speaker: Gyula Bencedi (Universidad Nacional Autonoma (MX))

Bencedi_LHCP2021.pdf

Zoom meeting room

240 ATLAS LAr Calorimeter Commissioning for LHC Run-3

Liquid argon (LAr) sampling calorimeters are employed by ATLAS for all electromagnetic calorimetry in the pseudo-rapidity region |η| < 3.2, and for hadronic and forward calorimetry in the region from |η| = 1.5 to |η| = 4.9. In the first LHC run a total luminosity of 27 fb$^{−1}$ has been collected at center-of-mass energies of 7-8 TeV. After detector consolidation during a long shutdown, Run-2 started in 2015 and about 150 fb$^{-1}$ of data at a center-of-mass energy of 13 TeV was recorded. With the end of Run-2 in 2018 a multi-year shutdown for the Phase-I detector upgrades was begun.
As part of the Phase-I upgrade, new trigger readout electronics of the ATLAS Liquid-Argon Calorimeter have been developed. Installation began at the start of the LHC shut down in 2019 and is expected to be completed in 2020. A commissioning campaign is underway in order to realize the capabilities of the new, higher granularity and higher precision level-1 trigger hardware in Run-3 data taking. This contribution will give an overview of the new trigger readout commissioning, as well as the preparations for Run-3 detector operation and changes in the monitoring and data quality procedures to cope with the increased pileup.

Speaker: Marcos Vinicius Silva Oliveira (CERN)

ATLAS LAr Calorimeter Commissioning for LHC Run-3 - LHCP2021 - Marcos Oliveira.pdf

Zoom meeting room

241 ATLAS searches extra dimensions for using the full Run 2 ee and mumu datasets

This poster summarises the extra dimensional models being searched for using the ATLAS detector at the Large Hadron Collider, in the full Run 2 dielectron and dimuon datasets. This data was produced in proton-proton collisions at a centre-of-mass energy of 13 TeV. In particular, the limits on the ADD model are presented, from a reinterpretation of the ATLAS Run 2 dilepton non-resonant analysis. Also highlighted, is a novel search being performed for clockwork extra dimensions.

Speaker: Tracey Berry (University of London (GB))

LHCPPosterADDBerry.pdf

Zoom meeting room

242 Charm is better than beauty: searching for the Higgs coupling to charm quarks

Eight years ago, the discovery of a new fundamental particle, the Higgs boson (H), was announced by the ATLAS and CMS collaborations at CERN. While elementary particles acquire their mass through their interaction with the Higgs field, the large differences in their masses as well as the origin of the three generations of fermions remain unexplained to this day and constitute the Standard Model flavour puzzle.
Measuring the coupling of each fermion to the Higgs boson is one of the most important tasks in modern particle physics. The next most promising candidate in the quark sector is the decay to a pair of charm quark and antiquark (cc).
This poster will focus on the analysis of the associated production of the Higgs boson with a W or Z boson performed by the ATLAS Collaboration using data collected between 2015 and 2018, and will describe the analysis strategy employed to search for the H→cc signal. More precisely, recent achievements in the charm tagging technology that enables the identification of jets containing charm hadrons will be presented. Our current understanding of the H→cc process will be outlined, and the various results of the ATLAS, CMS and LHCb collaborations will be compared. Finally, the interpretation of this new result as a probe to the Standard Model flavour puzzle and its large constraining power on new physics scenarios will be discussed.

Speaker: Marko Stamenkovic (Nikhef National institute for subatomic physics (NL))

LHCP_Poster_MarkoStamenkovic.pdf

LHCP_slides_MarkoStamenkovic.pdf

Video explanation

Zoom meeting room

243 CMS RPC activities during LS2 and Commissioning

The second LHC long shutdown period (LS2) was a crucial opportunity for the CMS Resistive Plate Chambers (RPC) to complete their consolidation and upgrade projects. The consolidation includes detector maintenance for gas tightness, HV (high voltage), LV (low voltage) and slow control operation. Dedicated studies were performed to understand the behaviour of RPC currents with comparison to RUN2. This paper summarises the activities performed and commissioning of CMS RPC on the surface (For RE4) and for full detector in CMS cavern in different operating conditions.

Speaker: Mapse Barroso Ferreira Filho (Universidade do Estado do Rio de Janeiro (BR))

Poster CMS RPC activities during LS2 and Commissioning - LHCP_2021.pdf

Zoom room link

244 Colour and logarithmic accuracy in final-state parton showers

Standard dipole parton showers are known to yield incorrect subleading-colour contributions to the leading (double) logarithmic terms for a variety of observables. In this work, concentrating on final-state showers, we present two simple, computationally efficient prescriptions to correct this problem, exploiting a Lund-diagram type classification of emission regions. We study the resulting effective multiple-emission matrix elements generated by the shower, and discuss their impact on subleading colour contributions to leading and next-to-leading logarithms (NLL) for a range of observables. In particular we show that the new schemes give the correct full colour NLL terms for global observables and multiplicities. Subleading colour issues remain at NLL (single logarithms) for non-global observables, though one of our two schemes reproduces the correct full-colour matrix-element for any number of energy-ordered commensurate-angle pairs of emissions. While we carry out our tests within the PanScales shower framework, the schemes are sufficiently simple that it should be straightforward to implement them also in other shower frameworks.

Speaker: Rok Medves (University of Oxford)

Colour Poster Medves LHCP2021

Poster video explanation

Zoom meeting room

245 Combined Constraints on First Generation Leptoquarks

We present a combined analysis of low energy precision constraints and LHC searches for leptoquarks which couple to first generation fermions. Considering all ten leptoquark representations, five scalar and five vector ones, we study at the precision frontier the constraints from $K\to\pi\nu\nu$, $K\to\pi e^+e^-$, $K^0-\bar K^0$ and $D^0-\bar D^0$ mixing, as well as from experiments searching for parity violation (APV and QWEAK). We include LHC searches for $s$-channel single resonant production, pair production and Drell-Yan-like signatures of leptoquarks. Particular emphasis is placed on the recent CMS analysis of lepton flavour universality violation in non-resonant di-lepton pairs. The excess in electron events could be explained by $t$-channel contributions of the leptoquark representations $\tilde{S}_1, S_2, S_3, \tilde{V}_1, V_2 (\kappa_2^{RL} \neq 0)$ and $V_3$ without violating other bounds. Regarding the so-called ``Cabibbo angle anomaly'', we observe that the present constraints are too restrictive to allow for a resolution via direct leptoquark contributions to super-allowed beta decays.

Speaker: Luc Schnell

Link to Zoom room

Poster (Landscape).pdf

Slides.pdf

Video Explanation.mp4

246 Constraining the Dark Sector with the Mono-jet signature with the ATLAS detector at the LHC

Several Dark Sector models predict the existence of particles with macroscopic life-times and semi-visible jets (QCD-like jets which include stable Dark Sector particles). These can lead to final states with large missing transverse momentum recoiling against at least one highly energetic jet, a signature that is often referred to as a mono-jet.
The RECAST framework is used to re-interpret the recent ATLAS mono-jet search, based on 139 $\mathrm{fb^{-1}}$ of pp collisions collision data at $\sqrt{s} = 13$ TeV, in terms of Dark Sector models not studied in the original work. Complementary results for models involving long-lived particles are found with respect to dedicated searches. Results are also interpreted for the first time at ATLAS in terms of searches for semi-visible jets produced from a QCD-like parton shower.

Speaker: Elena Pompa Pacchi (Sapienza Universita e INFN, Roma I (IT))

ConstrainingTheDarkSector_LHCP2021.pdf

Video Explanation

Zoom room link

247 Convolutional Neural Networks for event classification

In this study, a new technique for event classification using Convolutional Neural Networks (CNN) is presented. Results obtained using this technique are shown and compared to more traditional Machine Learning approaches for two different physics cases.
The new technique explores the power of visual recognition, which is one of the fastest-growing areas in Artificial Intelligence, as a consequence of the “deep learning” evolution of CNNs. Since CNNs are fed with images, an original and intuitive way for encoding the event information in images has been developed, building a one-to-one correspondence that allows us to face the event classification as an image classification.
In order to take advantage of the good performance of existing CNN architectures, transfer learning has been tested, showing to be a suitable option. VGG16 has been chosen as the benchmark, which is based on the well-known architecture named AlexNet. Additionally, an alternative approach with a simpler CNN architecture has shown to give also good results when trained from scratch. Nevertheless, a comparison with a more standard technique such as a BDT (using the XGBoost library) is provided in order to confirm that the results obtained with this unexplored technique are satisfactory.
The two classifications studied correspond to current challenges in Particle Physics. First, a New Physics example corresponding to a Dark Matter search has been performed, considering a mono-top signal and several of its main background processes. The selected events were required to have exactly one lepton and at least one b-tagged jet, together with large missing transverse momentum. Second, with the same selection criteria, a tt+X classification is also carried out, in which exotic processes with four top quarks as final state are tried to be identified among other processes such as ttH or ttW.

Speaker: Adrian Rubio Jimenez (Univ. of Valencia and CSIC (ES))

Adrian_LHCP_poster_2021.pdf

ADRIAN_LHCP_poster_video.mp4

Adrian_LHCP_slides_format_poster.pdf

Zoom meeting room

248 Correlation between initial spatial anisotropy and final momentum anisotropies in relativistic heavy ion collisions

The momentum anisotropy ($v_{n}$) of the produced particles in relativistic nuclear collisions is considered to be a response of the initial geometry or the spatial anisotropy ($\varepsilon_{n}$) of the system formed in these collisions. The linear correlation between $\varepsilon_{n}$ and $v_{n}$ measures the efficiency at which the initial spatial eccentricity is converted to final momentum anisotropy in heavy ion collisions. We have studied the transverse momentum, collision centrality, and beam energy dependence of this correlation for different charged particles using a hydrodynamical model framework MUSIC. The ($\varepsilon_{n}$ − $v_{n}$) correlation is found to be stronger for central collisions and also for n=2 compared to that for n=3 as expected. However, the transverse momentum ($p_{T}$) dependent correlation coefficient shows interesting behaviour which strongly depends on the mass as well as $p_{T}$ of the produced particles. The correlation strength is found to be larger for lighter particles in the lower $p_{T}$ region. We have seen that the relative fluctuation in anisotropic flow depends strongly in the value of $\eta/s$ specially in the region $p_{T}<$ 1 GeV unlike the correlation coefficient which does not show significant dependence on $\eta/s$

Speaker: Sanchari Thakur (Department of Atomic Energy (IN))

LHCP2021_sanchari_poster.pdf

sanchari_poster_LHCP.mp4

Zoom meeting room

249 Cosmics muon validation and electronics performance of the New Small Wheel MicroMegas sectors for ATLAS Muon Upgrade

The ATLAS Muon Upgrade project is a part of the Large Hadron Collider (LHC) - High Luminosity (HL) upgrade project which aims to increase its instantaneous luminosity up to 7.5X10$^{34}$ cm$^{−2}$s$^{−1}$. The present first muon station in the forward regions of ATLAS is being replace by the so-called New Small Wheels (NSWs). The NSWs consist of resistive-strip MicroMegas (MM) detectors and small-strip Thin Gap chambers (sTGC), both providing trigger and tracking capabilities, for a total active surface of more than 2500 m$^2$. After the R&D, design and prototyping phase, series production of MM and sTGC chambers are being constructed. The NSW Upgrade project, the most challenging and complex one of the ATLAS phase-I upgrade projects, is expected to be completed with the installation of NSW in the ATLAS Underground cavern during the summer of 2021. The whole NSW structure includes 128 detectors, in total to ∼2.4 million readout channels. This new generation of readout electronics are built to stand the harsh radiation hostile conditions, where the expected background rate will reach 20 kHz/cm$^2$. Eight micromegas detectors layers are integrated into a double wedge. The mechanical integration is followed by the electronic integration and its initial validation into the data acquisition system. Each fully equipped MicroMegas doublewedge is tested at a dedicated cosmic ray facility and the high voltage settings are defined. Then, a sequence of tests follows, related to efficiency maesurement , cluster size, resolution for all the individual layers of the double wedge are performed. These steps consist the qualification of the MicroMegas sector for the final integration with the sTGC wedges before mounting them on the NSW structure. The electronics performance and cosmic rays validation results of the final validation
of Micromegas double wedges will be presented.

Speaker: Maria Perganti (National Technical Univ. of Athens (GR))

Perganti_LHCP_2021_poster.pdf

Zoom meeting room

250 CP-violating observables and top-pair production at LHC.

We study new physics contributions to CP-violating anomalous couplings of top-quark in the context of top-pair production and their consequent decays into a pair of dilepton and b-jets at the Large Hadron Collider. An estimate of sensitivities to such CP-violating interactions would also be discussed for the pre-existing 13 TeV LHC data and its projections for the proposed LHC run at 14 TeV.

Speaker: Ms Apurba Tiwari (Aligarh Muslim University)

LHCP2021_poster.pdf

Zoom meeting room

251 Deep Neural Network resizing for real-time applications in High Energy Physics

Next-generation collider experiments will have to cope with extremely high collision rates, making it necessary to implement real-time event processing capabilities. Among the standard pattern recognition algorithms thought to be run on Look-Up Tables, Machine Learning methods, and in particular Deep Neural Networks, are spreading very fast and there is growing interest in executing such algorithms at trigger level to improve on-line selection performance. The main issue in running these algorithms in real-time is the amount of operation that needs to be computed. Low-latency hardware solutions exist, e.g. FPGAs, but the main constraint to the implementation is often related to the size of the model, that has to be finely tuned not to exceed the available memory. We present an approach to reduce in an optimized way the size of models based on Fully Connected Neural Networks, having under control the model performances. The number of features in input to the Deep Neural Network is reduced using a CancelOut layer, optimized through an original loss function. We compare the performances of this approach with other techniques. We use as baseline study the selection of proton-proton collision events in which the boosted Higgs boson decays to two $b$-quarks and both the decay products are contained in a large and massive jet. These events have to be selected against an overwhelming QCD background. Promising results are shown and the way for future developments is outlined.

Speaker: Mr Andrea Di Luca (Universita degli Studi di Trento and INFN (IT))

Deep Neural Network resizing for real-time applications in High Energy Physics-lhcp2021_poster.pdf

Zoom meeting room

252 Development of a L1 tau trigger algorithm using the CMS high-granularity calorimeter information

The High-Luminosity LHC will open an unprecedented window on the weak-scale nature of the universe, providing high-precision measurements of the Standard Model (SM) as well as searches for new physics beyond the SM. The CMS Collaboration is planning to replace entirely its trigger and data acquisition systems to match this ambitious physics program. Efficiently collecting datasets in Phase 2 will be a challenging task, given the harsh environment of 200 proton-proton interactions per LHC bunch crossing. The already challenging implementation of an efficient tau lepton trigger will become, in this conditions, an even crucial and harder task; especially interesting will be the case of hadronically decaying taus. To this end, the foreseen high-granularity endcap calorimeter (HGCAL), and the astonishing amount of information it will provide, play a key role in the design of the new online level-1 (L1) triggering system. In this talk I will present the development of a L1 trigger for hadronically decaying taus based on the sole information from the HGCAL detector. I will present some novel ideas for a L1 trigger based on machine learning that can be implemented in FPGA firmware. The expected performance of the new trigger algorithm will be presented, based on simulated collision data of the HL-LHC.

Speaker: Mr Jona Motta (Centre National de la Recherche Scientifique (FR))

L1TauTrg_poster.pdf

L1TauTrg_slides.pdf

video.mov

video.mp4

Zoom meeting room

253 Development of DAQ to DCS communication in the ATLAS Inner Tracker

The increase of luminosity foreseen for the High-Luminosity LHC phase requires the substitution of the ATLAS Inner Detector with a new tracking detector, called Inner Tracker. It will be an all-silicon system consisting of a pixel and a strip subdetector. The ATLAS wide FELIX system will be the off-detector interface to the Inner Tracker.
In order to efficiently bring the Inner Tracker into operation, the intercommunication between the DAQ and the DCS is foreseen. Such communication is mediated by OPC servers that interface to the different hardware and software resources and to the Finite State Machine, which supervises all subdetectors. This framework is designed to be flexible, so that it can easily incorporate heterogeneous resources coming from different subsystems, including the FELIX setups.
This poster describes the current status of the implementation of OPC servers for the intercommunication between the DAQ and the DCS and their integration in the FELIX setups.

Speaker: Alessandra Palazzo (INFN Lecce e Universita del Salento (IT))

DAQtoDCSCommunicationITk.pdf

Poster video explanation

Zoom room

254 Development of the ATLAS Liquid Argon Calorimeter Readout Electronics for the HL-LHC

To meet new TDAQ buffering requirements and withstand the high expected radiation doses at the high-luminosity LHC, the ATLAS Liquid Argon Calorimeter readout electronics will be upgraded. The triangular calorimeter signals are amplified and shaped by analogue electronics over a dynamic range of 16 bits, with low noise and excellent linearity. Developments of low-power preamplifiers and shapers to meet these requirements are ongoing in 130nm CMOS technology. In order to digitize the analogue signals on two gains after shaping, a radiation-hard, low-power 40 MHz 14-bit ADCs is developed using a pipeline+SAR architecture in 65 nm CMOS. Characterization of the prototypes of the frontend components show good promise to fulfill all the requirements. The signals will be sent at 40 MHz to the off-detector electronics, where FPGAs connected through high-speed links will perform energy and time reconstruction through the application of corrections and digital filtering. Reduced data are sent with low latency to the first level trigger, while the full data are buffered until the reception of trigger accept signals. The data-processing, control and timing functions will be realized by dedicated boards connected through ATCA crates. Results of tests of prototypes of front-end components will be presented, along with design studies on the performance of the off-detector readout system.

Speaker: Mesut Unal (University of Texas at Austin (US))

Unal-ATL-COM-PHYS-2021-309.2.pdf

Video_Explanation

Zoom meeting room

255 Development of the Configuration, Calibration and Monitoring System of the New Small Wheel Electronics for the ATLAS experiment

A series of upgrades are planned for the LHC accelerator to increase it's instantaneous luminosity to 7.5×10$^{34}$ cm$^{-2}$s$^{-1}$. The luminosity increase drastically impacts the ATLAS trigger and readout data rates. The present ATLAS Small Wheel Muon detector will be replaced with a New Small Wheel (NSW) detector which is expected to be installed in the ATLAS underground cavern by the end of the Long Shutdown 2 of the LHC. One crucial part of the integration procedure concerns the installation, testing and validation of the on-detector electronics and readout chain for a very large system with a more than 2.1 M electronic channels in total. These include 7K Front-End Boards (MMFE8, SFEB, PFEB), custom printed circuit boards each one housing eight 64-channel VMM Application Specific Integrated Circuits (ASICs) that interface with the ATLAS Trigger and Data Acquisition (TDAQ) system through 1K data-driver cards. The readout chain is based on optical link technology (GigaBit Transceiver links) connecting the backend to the front-end electronics via the Front-End LInk eXchange (FELIX), is a newly developed system that will serve as the next generation readout driver for ATLAS. For the configuration, calibration and monitoring path, the various electronics boards are supplied with the GBT-SCA ASIC (Giga-Bit Transceiver-Slow Control Adapter) which is part of the Gigabit Transceiver Link(GBT) chipset and it's purpose is to distribute control and monitoring signals to the electronics embedded in the detectors and in the ATLAS service areas. Experience and performance results from the first large-scale electronics integration tests performed at CERN on final NSW sectors will be presented.

Speaker: Polyneikis Tzanis (National Technical Univ. of Athens (GR))

tzanis_poster_lhcp_2021.pdf

Zoom Room

256 Differential cross section measurements of the tW process at CMS

Single top quark production is the subleading production process of top quarks at the LHC after the top quark pair production. The latest differential measurements of single top quark production (tW) cross sections are presented using data collected by the CMS detector at a center-of-mass energy of 13 TeV. The cross sections are measured as a function of various kinematic observables of the top quarks and the jets and leptons of the events in the final state. The results are confronted with precise theory calculations.

Speaker: Mr Victor Rodriguez Bouza (Universidad de Oviedo - ICTEA (ES))

2021-06_lhcp_tWdiffposter.pdf

Zoom meeting room

257 Event-Level Anomaly Detection for Multijet BSM Searches with Probabilistic Autoencoders

Although most of Beyond Standard Model (BSM) searches are targeting specific theory models, there has always been a keen interest in the development of model-independent methods amongst the High Energy Physics(HEP) community. Machine Learning (ML) based anomaly detection stands among the latest up-and-coming avenues for creating model-agnostic BSM searches. The focus of this research is the design of anomalous event taggers based on autoencoder models. Alongside the signal discrimination power, a high priority is placed on both signal-model and background-model independence. To this end, the autoencoder is used in conjunction with a Normalizing Flow model tasked with latent space density estimation. Both event reconstruction error and latent representation likelihood are combined in order to mitigate the bias of the resulting event anomaly score. Overall this method is showing promising anomaly detection performance without loosing much in terms of generalization power. On the multijet LHC Olympics data, it is consistently able to identify BSM signals, even in the challenging scenarios posed by the Black Box datasets, where the signal content is unknown.

Speaker: Ioan-Mihail Dinu (Horia Hulubei National Institute of Physics and Nuclear Enginee)

DINU_LHCP2021_landscape.pdf

DINU_LHCP2021.pdf

Zoom Meeting Room

258 Evidence for four-top-quark production in the multilepton final state in proton-proton collisions at sqrt(s)=13 TeV with the ATLAS detector

A search is presented for four-top-quark production using proton-proton collision data at a centre-of-mass energy of 13 TeV collected by the ATLAS detector at the Large Hadron Collider with an integrated luminosity of 139/fb. Events are selected if they contain a same-sign lepton pair or at least three leptons (electrons or muons). Jet multiplicity, jet flavour and event kinematics are used to separate signal from the background through a multivariate discriminant, and dedicated control regions are used to constrain the dominant backgrounds. The four-top-quark production cross section is measured to be 24 +7 -6 fb. This corresponds to an observed (expected) significance with respect to the background-only hypothesis of 4.3 (2.4) standard deviations and provides evidence for this process.

Speaker: Albert Kong (University of Adelaide (AU))

lhcp2021-poster.pdf

Zoom meeting room

259 Extension of Glauber-like model for Proton-Proton collisions using anisotropic and inhomogeneous density profile

The formation of partonic medium in the relativistics heavy-ion collisions is always marked by the values of the ratio of certain observables assuming $p+p$ collisions as a reference. But recent studies of small systems formed in $p+p$ collisions at the LHC energies hint towards the possibility of production of medium with collective behaviour. Results from $p+p$ collisions have routinely been used as baseline to analyse and understand the production of QCD matter expected to be produced in nuclear collisions. Therefore, results from $p+p$ collisions required more careful investigation to understand whether QCD matter is produced in high multiplicity $p+p$ collisions. With this motivation, the Glauber model traditionally used to study the heavy-ion collision dynamics at high-energies is applied to understand the dynamics of $p+p$ collisions. We have used anisotropic and inhomogeneous quark/gluon based proton density profile, a realistic picture obtained from the results of deep inelastic scattering, and found that this model explains the charged-particle multiplicity distribution of $p+p$ collisions at LHC energies very well. Collision geometric properties like impact parameter and mean number of binary collisions ($\langle N_{coll} \rangle$), mean number of participants ($\langle N_{part} \rangle$) at different multiplicities are determined for $p+p$ collisions. We further used these collision geometric properties to estimate average charged-particle pseudorapidity density ($\langle dN_{ch}/d\eta \rangle$) and found it to be comparable with the experimental results. Knowing $\langle N_{coll} \rangle$, we have for the first time obtained nuclear modification-like factor ($R_{HL}$) in $p+p$ collisions. We also estimated eccentricity and elliptic flow as a function of charged-particle multiplicity using the linear response to initial geometry and found a good agreement with experimental results.

Speaker: Suman Deb (Indian Institute of Technology Indore (IN))

LHCP_Suman_Glauber.pdf

Zoom meeting room

260 Extraction of the multiplicity dependence of Multiparton Interactions from LHC pp data using Machine Learning techniques

Over the last years, Machine Learning (ML) tools have been successfully applied to a wealth of problems in high-energy physics. In this talk, we will discuss the extraction of the average number of Multiparton Interactions ($〈N_{mpi}〉$) from minimum-bias pp data at LHC energies using ML methods. Using the available ALICE data on transverse momentum spectra as a function of multiplicity we report the $〈N_{mpi}〉$ for pp collisions at √s = 7 TeV, which complements our previous results for pp collisions at √s = 5.02 and 13 TeV. The comparisons indicated a modest energy dependence of $〈N_{mpi}〉$. We also report the multiplicity dependence of $N_{mpi}$ for the three center-of-mass energies. These results are fully consistent with the existing ALICE measurements sensitives to MPI, therefore they provide experimental evidence of the presence of MPI in pp collisions.

Speaker: Erik Alfredo Zepeda Garcia (Universidad Nacional Autonoma (MX))

LHCP2021erik.pdf

Zoom meeting room

261 Fast Beam Condition Monitor of the CMS experiment for precision luminosity measurement at HL-LHC

To achieve the challenging target of 1% precision on luminosity determination at the high-luminosity LHC (HL-LHC) with instantaneous luminosity up to $7.5 × 10^{34} cm^{−2} s^{−1}$, the CMS experiment will employ multiple luminometers with orthogonal systematics. A key component of the proposed system is a stand-alone luminometer, the Fast Beam Condition Monitor (FBCM), which is fully independent from the central trigger and data acquisition services and able to operate during all times at 40 MHz providing bunch-by-bunch luminosity measurement with 1 s time granularity. FBCM is foreseen to be placed inside the cold volume of the Tracker as it utilizes silicon-pad sensors exploiting the zero-counting algorithm of hits for luminosity measurement. FBCM will also provide precise timing information with a few ns precision enabling the measurement of beam induced background. We report on the optimization of the design and the expected performance of FBCM.

Speaker: Hamed Bakhshiansohi (DESY and IUT)

FBCMPosterLHCP2021.pdf

Zoom meeting room

262 Fast simulation of a Time-of-Flight detector for Forward Protons at the LHC

The ATLAS Forward Proton physics program at CERN aims at studying soft and hard diffractive events from ATLAS proton collisions. Time-of-Flight (ToF) system is used to reduce the background from multiple proton-proton collisions. In this presentation, we describe technical details of the Fast Cherenkov model of photons generation and transportation through the optical part of the ToF detector. This Fast simulation uses Python programming language and Numba (high performance compiler). It is about 200 times faster than Geant4 simulation already implemented, and provides similar results concerning length and time distributions of photons. Moreover, this Fast simulation allows computing easily the time resolution of the different bars of ToF detector.

Speaker: Olivier Rousselle (Laboratoire Kastler Brossel (FR))

Fast simulation - Olivier Rousselle.pdf

ZOOM poster room

263 FELIX-based Data Acquisition System Integration with the NSW Micromegas Electronics and Detector Performance Validation

The New Small Wheel (NSW) upgrade is now in its commissioning phase. The future ATLAS detector sub-system will be one of the first to employ the Front-End Link eXchange (FELIX) as its Data Acquisition (DAQ) scheme. Currently, one of the main focus points of the community is to ensure proper acquiring of data from the detector media, besides validating the performance of the detectors themselves. This is being conducted at the BB5 area of CERN, where the Micromegas chambers are subjected to cosmic radiation. In this work, the software and FPGA-based tools that have been developed to aid in satisfying the stringent 2-week turnaround time per detector wedge will be described. These include applications that control the complex DAQ system and validate the data paths of thousands of readout channels and hundreds of high-speed optical links in an automated manner. Another aspect of the work is the description of methodologies that have been developed to validate the chamber’s performance under cosmic radiation. Finally, an FPGA system that performs scintillator coincidence trigger filtering will be described. The aforementioned part of the system is used to emulate the deterministic nature of the muons’ time-of-arrival during the actual run, in order to perform timing resolution performance profiling of the Micromegas detector.

Speaker: Christos Bakalis (National Technical Univ. of Athens (GR))

lhcp_poster_bakalis.pdf

Zoom Meeting Room

264 Femtoscopic analysis of $\mathrm{K^0_S-p}$ pairs in proton–proton collisions at $\sqrt{s} = 13$ TeV with ALICE

The precise knowledge of the strong interaction between kaons and nucleons
is a key element to describe the interaction between hadrons in the non-perturbative regime of QCD.
Moreover, the knowledge of this interaction plays an important role in the study of the equation
of state of dense baryonic matter, and hence has important implications for the
modeling of neutron stars.

We present the first femtoscopy measurement of momentum correlations of $\mathrm{K^0_Sp}$ and $\mathrm{K^0_S\overline{p}}$ pairs in pp collisions at $\sqrt{s}=13 $ TeV measured by the ALICE experiment at the LHC.
In this study, the strong scattering parameters of $\mathrm{K^0_Sp}$ and $\mathrm{K^0_S\overline{p}}$ pairs are extracted through the Lednicky-Lyuboshitz model. This model links the experimental momentum correlation to the strong final state interaction parameters.
The extracted scattering parameters indicate that the strong interaction between $\mathrm{K^0_Sp}$($\mathrm{\overline{p}}$) is attractive, contrary to $\mathrm{K^+p}$ and $\mathrm{K^-p}$. This indicates that in the $\mathrm{K^0_Sp}$($\mathrm{\overline{p}}$)
there are no resonances below threshold which are responsible of the repulsive strong interaction between $\mathrm{K^-p}$.

Speaker: Marta Urioni (Universita di Brescia (IT))

K0sp_femto_ALICE_LHCP2021.pdf

Zoom Meeting Room

265 Firmware of the ATLAS Level-0 Endcap Muon Trigger for HL-LHC

The design and the status of the development of the Level-0 endcap muon trigger firmware for the ATLAS experiment at the HL-LHC are presented. The firmware reconstructs muon candidates with an improved momentum resolution by exploiting all hit data from Thin Gap Chambers (TGCs) to be available at XCVU13P FPGA mounted on the trigger and readout boards. The track segment is reconstructed by a pattern matching algorithm, where the TGC hits are compared with predefined hit patterns. Each predefined hit pattern has associated position and angle of the track segment. The algorithm with minimal utilisation of the XCVU13P FPGA resource is a major challenge. We achieved 1 cm position and 4 mrad angular resolutions, which satisfy the requirements, with less than 40% of the UltraRAM resources for full coverage of TGCs. The performance was evaluated with the post-synthesis simulation with the hit inputs from GEANT4 full simulation. The implementation was succeeded with no timing violation by optimised latch circuit locations. The results constitute an important ingredients in the development of the Level-0 endcap muon trigger firmware for HL-LHC.

Speaker: Yuki Mitsumori (Nagoya University (JP))

Firmware_of_the_ATLAS_Level-0_Endcap_Muon_Trigger_for_HL-LHC.pdf

ZOOM meeting room

266 First Commissioning Data from FASER

FASER (ForwArd Search ExpeRiment) fills the axial blindspot of other, radially arranged LHC experiments. It is installed 480 meters from the ATLAS interaction point, along the collision axis. FASER will search for dark matter and other new, long-lived particles that may be hidden in the collimated reaction products exiting ATLAS. FASER comprises: a magnetic spectrometer built with ATLAS silicon tracker modules; four LHCb outer ECAL modules; an emulsion neutrino detector; and plastic scintillators for veto, trigger and timing. The experiment is currently in its final commissioning stages. I report on successful preliminary tests of hardware and software performance with cosmic rays on the surface, and after installation in situ. FASER will begin taking pp collision data from the start of LHC Run 3, in 2022.

Speaker: Savannah Rose Shively (University of California Irvine (US))

LHCP - Shively - FASER Commissioning.pdf

Zoom meeting room

267 Hyperloop – The ALICE analysis train system for Run 3

ALICE analysis mostly deals with large datasets using the distributed Grid infrastructure. In Run 1 and 2, ALICE developed a system of analysis trains (so-called “LEGO trains”) that allowed the user to configure analysis tasks (or wagons) that are expected to be run on the same data. The LEGO train system builds upon existing tools: the ALICE analysis framework as well as the Grid submission and monitoring infrastructure. This centralized system improved the resource utilization and provided a friendly user interface (UI), in addition to bookkeeping functionalities. Currently, 90$\%$ of ALICE analyses use the train system. The ongoing major upgrade for LHC Run 3 will enable the experiment to cope with an increase of lead-lead collision data of two orders of magnitude compared to the Run 1 and 2 data-taking periods. In order to process this unprecedented data sample, a new computing model has been implemented, the Online-Offline Computing System (O$^2$). Analysis trains will also be the main workhorse for analysis in Run 3: a new infrastructure, Hyperloop, is being developed based on the successful concept of the LEGO trains. The Hyperloop train system includes a different and improved UI using modern responsive web tools, bookkeeping, instantaneous automatic testing, and the production of derived skimmed data. So far, about 600 Hyperloop trains have been successfully submitted to the Grid and ALICE analysis facilities using converted Run 2 data. An overview of ALICE train system concept will be exposed in this poster, highlighting the improvements of the new Hyperloop framework for analysis in Run 3.

Speaker: Raquel Quishpe Quishpe (University of Houston (US))

Poster video explanation

Quishpe-LHCP-Poster.pdf

Zoom meeting room

268 Impact of Soft Photons on $B\to K\ell^+\ell^-$

In this talk, we will be discussing $\mathcal{O}(\alpha)$ QED corrections to $B\to K\ell^+\ell^-$ modes. The structure of the contact term is fixed by requiring the gauge invariance of the real emission amplitude. The calculation is done by providing fictitious mass ($\lambda$) to the photon, which acts as IR regulator and results are shown to be independent of it. QED effects are found to be negative. Electron channels are shown to receive large correction $\mathcal{O}(20\%)$. We will also discuss its impact on lepton flavour universality (LFU) ratio ($R_{K}^{\mu e}$).

Speaker: Dayanand Mishra

LHCP2021 .pdf

Poster introduction

Zoom meeting room

269 Implementation of machine learning techniques to predict impact parameter and transverse spherocity in heavy-ion collisions at the LHC

Machine learning techniques have been quite popular recently in the high-energy physics community and have led to numerous developments in this field. In heavy-ion collisions, one of the crucial observables, the impact parameter, plays an important role in the final-state particle production. This being extremely small (i.e. of the order of a few fermi), it is almost impossible to measure impact parameter in experiments. In this work, we implement the ML-based regression technique via Gradient Boosting Decision Trees (GBDT) to obtain a prediction of impact parameter in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV using A Multi-Phase Transport (AMPT) model. After its successful implementation in small collision systems, transverse spherocity, an event shape observable, holds an opportunity to reveal more about the particle production in heavy-ion collisions as well. In the absence of any experimental exploration in this direction at the LHC yet, we suggest an ML-based regression method to estimate centrality-wise transverse spherocity distributions in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV by training the model with minimum bias collision data. Throughout this work, we have used a few final state observables as the input to the ML-model, which could be easily made available from collision data. Our method seems to work quite well as we see a good agreement between the simulated true values and the predicted values from the ML-model.

Speaker: Dr Aditya Nath Mishra (Wigner Research Centre for Physics Budapest, Hungary)

Implementation of machine learning techniques to predict impact parameter and transverse spherocity in heavy-ion collisions at the LHC

Poster-ML-Aditya.pdf

270 Inclusive top-antitop production cross section at sqrt(s) = 5.02 TeV in CMS

The top quark pair production cross section is measured in proton-proton collisions at a center-of-mass energy of 5.02 TeV. The data collected in 2017 by the CMS experiment at the LHC corresponding to an integrated luminosity of 304 1/pb are analyzed. The measurement is performed using events with one electron and one muon of opposite sign, and at least two jets. The measured cross section is found to be 60.3 ± 5.0 (stat) ± 2.8 (syst) ± 0.9 (lumi) pb. To reduce the statistical uncertainty, a combination with the result in the l+jets channel, based on 27.4 1/pb of data collected in 2015 at the same center-of-mass energy, is then performed, obtaining a value of 62.6 ± 4.1 (stat) ± 3.0 ( syst+lumi ) pb, with a total uncertainty of 7.9%, in agreement with the standard model.

Speaker: Alejandro Soto Rodriguez (Universidad de Oviedo (ES))

LHCP-ttbar5TeV.pdf

Zoom meeting room

271 Insight into K∗ production in pp collisions as a function of collision energy, event-topology and multiplicity with ALICE at the LHC

Hadronic resonances are short-lived particles whose lifetimes are comparable to the hadronic phase lifetime of the system produced in ultrarelativistic nucleon-nucleon or nuclear collisions. These resonances are sensitive to the hadronic phase effects such as rescattering and regeneration processes which might affect the resonance yields and shape of the transverse momentum spectra. In addition, event shape observables like transverse spherocity are sensitive to the hard and soft processes. They are useful tools to distinguish the isotropic and jetty-dominated events in pp collisions. Studying the dependence of the yield of resonance on transverse spherocity and multiplicity allows us to understand the resonance production mechanism with event topology and system size respectively. Furthermore, the measurements in small systems are used as a reference for heavy-ion collisions and are helpful for the tuning of Quantum chromodynamics inspired event generators. In this contribution, we present recent results on K∗(892)0 production obtained by the ALICE experiment in pp collisions at several collision energies, event multiplicities and as a function of transverse spherocity. The results include the transverse momentum spectra, yields and their ratio to the yields of long-lived particles. The measurements done using the ALICE detector will be compared with the corresponding results from models such as PYTHIA8, EPOS-LHC etc., and the measurements at lower energies.

Speaker: Rutuparna Rath (Indian Institute of Technology Indore (IN))

LHCP2021-Rutuparna-10June2021.pdf

Zoom meeting link

272 LCSR application to radiative tau decay

The non-perturbative QCD effects involved in radiative tau decay $(\tau^- \rightarrow \pi^- \nu_\tau \gamma)$ are encoded in two form factors; the vector ($F_V$) and the axial vector ($F_A$) form factors. We present the computation of these form factors using light cone sum rules. The form factors involved in this decay are same as involved in radiative pion decay with the crucial difference that the momentum transfer squared, $t$, between the pion-photon system is positive, which makes these form factors timelike and also as $t$ can now take values up to $m_\tau^2$, it can produce real hadronic resonances. We calculate the analytical form for these form factors using the method of light cone sum rules and present the decay width and the invariant mass spectrum in the $\pi-\gamma$ system. We found that the structure dependent parameter, $\gamma$, i.e. the ratio of the axial vector to vector form factor at zero momentum transfer to be in good agreement with the experimental determination.

Speaker: Anshika Bansal (Physical Research Laboratory, Ahmedabad)

LHCP21_Poster_anshika.pdf

Poster video explanation

Zoom meeting room

273 LFUV Tests at the Z Pole

$b\to s\tau\tau$ and $b\to c\tau \nu$ measurements are highly motivated for addressing lepton-flavor-universality-violating (LFUV) puzzles, such as $R_{D^{(*)}}$, $R_{J/\psi}$ and $R_{K^{(\ast)}}$ anomalies, raised by the data of LHCb, BELLE and BarBar. The planned operation of future $e^-e^+$ colliders as a $Z$ factory provides a great opportunity to conduct such measurements, because of its relatively high production rates and reconstruction efficiency for $B$ mesons at $Z$ pole. Here we will pursue a systematic sensitivity study on these measurements at future $Z$ factories. The implications of the outcomes for LFUV new physics will be also explored.

Speaker: LINGFENG LI (HKUST)

LFU_Tests_at_the_Z_Pole_Full_Poster.pdf

LFU Tests at the Z Pole.mp4

LFU_Tests_at_the_Z_Pole_Small_Poster.pdf

Zoom Meeting Room

274 Luminosity and beam-induced background measurement with the CMS tracker endcap pixel detector at HL-LHC

The High Luminosity upgrade of the LHC (HL-LHC) places unprecedented requirements for background monitoring and luminosity measurements. The CMS Tracker Endcap Pixel Detector (TEPX) will be adapted to provide high-precision online measurements of bunch-by-bunch luminosity and beam-induced background. The implementation of dedicated triggering and readout systems, the real-time clustering algorithm on an FPGA and the expected performance are discussed. The innermost ring of the last layer (D4R1) will be operated independently from the rest of TEPX enabling beam monitoring during the LHC ramp and during unqualified beam conditions. The system optimisation and the dedicated timing and trigger infrastructure for D4R1 are also presented.

Speaker: Peter Kicsiny (KIT - Karlsruhe Institute of Technology (DE))

LHCP21_poster.pdf

LHCP21_slides.pdf

Zoom meeting room

275 Luminosity measurement at muon collider

The precise determination of the luminosity in a collider is of crucial importance for any physics cross sections measurement since it directly translates to the precision of the cross section determination.
In a muon collider dense muon beams are necessary to achieve the target luminosity, these beams generate very high fluxes of particles coming from the muons decay along the beam pipe.
Due to the presence of ad-hoc shielding structure, designed to mitigate the effect of the beam-induced background, the forward region of the detector cannot host instrumentation for the determination of the luminosity, as in standard methods adopted by the LHC experiments.
In this poster an alternative way to determine such a fundamental parameter is proposed, taking inspiration from flavour factories such as Belle2 and BES, where the luminosity is measured by counting $e^+$ $e^-$ $\to$ $e^+$ $e^-$ Bhabha events, whose cross-section is theoretically known with high precision.
The reconstruction efficiency of large angle muon Bhabha ($\mu^+$ $\mu^-$ $\to$ $\mu^+$ $\mu^-$) events at 1.5 TeV center of mass energy is estimated at muon collider via full detector simulation, taking into account the beam-induced background effects.
Kinematic requirements are defined to optimize the signal to physics background ratio and the statistical uncertainty on the muon collider luminosity measurement that can be reached with this method is estimated.

Speakers: Carlo Giraldin (University of Padova), Laura Buonincontri (Universita e INFN, Padova (IT))

Luminosity measurement at Muon Collider​.pdf

Poster video explanation

Zoom meeting room

276 LUXE: A new experiment to study non-perturbative QED in electron-LASER and photon-LASER collisions

The LUXE experiment (LASER Und XFEL Experiment) is a new experiment in planning at DESY Hamburg using the electron beam of the European XFEL. LUXE is intended to study collisions between a high-intensity optical LASER and 16.5 GeV electrons from the XFEL electron beam, as well as collisions between the optical LASER and high-energy secondary photons. The physics objective of LUXE are processes of Quantum Electrodynamics (QED) at the strong-field frontier, where the electromagnetic field of the LASER is above the Schwinger limit. In this regime, QED is non-perturbative. This manifests itself in the creation of physical electron-positron pairs from the QED vacuum, similar to Hawking radiation from black holes. LUXE intends to measure the positron production rate in an unprecedented LASER intensity regime. An overview of the LUXE experimental setup is given, in the context within the field of high-intensity particle physics. The foreseen detector systems and their sensitivity are presented. Finally, the prospects for studying BSM physics are also discussed.

Speaker: Federico Meloni (Deutsches Elektronen-Synchrotron (DE))

LHCp2021_poster.pdf

Zoom meeting room

277 Mass Unspecific Supervised Tagging (MUST) for boosted jets

Jet identification tools are crucial for new physics searches at the LHC and at future colliders. We introduce the concept of Mass Unspecific Supervised Tagging (MUST) which relies on considering both jet mass and transverse momentum varying over wide ranges as input variables - together with jet substructure observables - of a multivariate tool. This approach not only provides a single efficient tagger for arbitrary ranges of jet mass and transverse momentum, but also an optimal solution for the mass correlation problem inherent to current taggers. By training neural networks, we build MUST-inspired generic and multi-pronged jet taggers which, when tested with various new physics signals, clearly outperform the variables commonly used by experiments to discriminate signal from background. These taggers are also efficient to spot signals for which they have not been trained. Taggers can also be built to determine, with a high degree of confidence, the prongness of a jet, which would be of utmost importance in case a new physics signal is discovered.

Speaker: João Seabra (Instituto Superior Técnico)

MUST_LHCP2021.mp4

Poster_LHCP2021.pdf

Zoom meeting room

278 Measurement of $\mathrm{D}$-meson production as a function of charged-particle multiplicity in proton-proton collisions at $\sqrt{s} = 13$ TeV with ALICE at the LHC

Heavy quarks (charm and beauty) are produced at the initial stages of the relativistic hadronic collisions in hard scattering processes, and the study of their production in proton-proton (pp) collisions is an important test for calculations based on perturbative Quantum Chromodynamics (pQCD). Analysis of heavy flavor production as a function of charged-particle multiplicity provides insight into the processes occurring at the partonic level and the interplay between the hard and soft particle production mechanisms in pp collisions.

In this poster, measurements of open heavy-flavor production as a function of multiplicity, via the study of the $\mathrm{D}$-meson self-normalized yields in pp collisions at the center-of-mass energy of $\sqrt{s} = 13$ TeV is presented. The $\mathrm{D}$-meson yields are measured in different $p_{\rm{T}}$ intervals from 1 GeV/$c$ to 24 GeV/$c$ at midrapidity via their hadronic decay channels. The $\mathrm{D}$-meson self-normalized yield is found to increase stronger than linearly with increasing charged-particle multiplicity. The measurements are compared to PYTHIA 8 calculations, and with the results at $\sqrt{s} = 7$ TeV.

Speaker: Yoshini Bailung (Indian Institute of Technology Indore (IN))

LHCP2021_Yoshini_v7.pdf

Zoom meeting room

279 Measurement of Bc(2S) and Bc(2S)* cross section ratios in proton-proton collisions at 13 TeV

The ratios of the Bc(2S) to Bc, Bc(2S) to Bc, and Bc(2S) to Bc(2S) production cross sections are measured in proton-proton collisions at 13 TeV, using a data sample collected by the CMS experiment at the LHC, corresponding to an integrated luminosity of 143 fb−1. The three measurements are made in the Bc meson phase space region defined by the transverse momentum pT > 15 GeV and absolute rapidity |y| < 2.4, with the excited Bc(2S) states reconstructed through the Bc π+π−, followed by the Bc → J/ψπ+ and J/ψ → μ+μ− decays. The Bc(2S) to Bc, Bc(2S) to Bc, and Bc(2S) to Bc(2S) cross section ratios, including the unknown Bc(2S) → Bcπ+π− branching fractions, are (3.47 ± 0.63 (stat) ± 0.33 (syst))%, (4.69 ± 0.71 (stat) ± 0.56 (syst))%, and 1.35 ± 0.32 (stat) ± 0.09 (syst), respectively. None of these ratios shows a significant dependence on the pT or |y| of the Bc meson. The normalized dipion invariant mass distributions from the decays Bc(2S) → Bc π+π− are also reported.

Speaker: Manuel Alejandro Rodriguez Giraldo (Universidad de Antioquia (CO))

ManuelRodriguezlhcp2021.pdf

Zoom meeting room

280 Measurement of Higgs boson production in association with a W or Z boson in the H->WW decay channel

Recent measurements of the Higgs boson production cross section in the H->WW decay channel using proton-proton collision data with CMS experiment at 13 TeV will be presented. In particular the Higgs boson production in association with leptonically decaying vector bosons is targeted, and the H->WW decays in which at least one W boson decays to leptons are considered. Results for both the inclusive production cross section and cross sections in the STXS scheme will be presented.

Speaker: Ms Sahithi Rudrabhatla (On behalf of the CMS Collaboration )

lhcp 2021- page all final (1).pdf

Zoom meeting room

281 Measurement of the CP structure of the Yukawa interaction in Higgs boson decays to tau leptons in CMS

The discovery of the Higgs boson in 2012 by the CMS and ATLAS collaborations marked the start of the exploration of the Higgs sector of particle physics. The properties of the Higgs sector under CP symmetry have been investigated mostly in its couplings to gauge bosons. With the full Run 2 data-taking period it became possible to study the CP properties of the Yukawa coupling of the Higgs to fermions, and in particular to tau leptons. This was done reconstructing the decay planes of the two tau leptons and measuring their angular correlation. The measured mixing angle between CP-even and CP-odd couplings is (4±17)° and is consistent with the Standard Model prediction of a pure CP-even coupling and allows to constrain the allowed phase space for possible BSM scenarios. A pure CP-odd hypothesis is instead excluded with 99.7% confidence level.

Speaker: Andrea Cardini (Deutsches Elektronen-Synchrotron (DE))

Poster-full-AndreaCardini-LHCP2021.pdf

Poster-split-AndreaCardini-LHCP2021.pdf

Slides-AndreaCardini-LHCP2021.pdf

Video-PanelDescription.mp4

Zoom meeting room

282 Measurement of the four-top-quark production cross section in pp collisions at sqrt(s)=13 TeV with the ATLAS detector

A measurement of four-top-quark production using proton-proton collision data at a centre-of-mass energy of 13 TeV collected by the ATLAS detector at the Large Hadron Collider with an integrated luminosity of 139/fb is presented. A new result uses events with a single lepton (electron or muon) or an opposite-sign lepton pair, in association with multiple jets. The measured four-top-quark production cross section is found to be 26 +17 -15 fb, with a corresponding observed (expected) significance of 1.9 (1.0) standard deviations over the background-only hypothesis. The result is combined with the previous measurement performed by the ATLAS Collaboration in the multilepton final state. The combined four-top-quark production cross section is measured to be 25 +7 -6 fb, with a corresponding observed (expected) signal significance of 4.7 (2.6) standard deviations over the background-only predictions. The result is consistent within 2.0 standard deviations with the Standard Model expectation of 12.0 +/- 2.4 fb.

Speaker: Martin Murin (University of Manchester (GB))

Poster-Slides_LHCP2021_4top_Murin.pdf

Zoom meeting room

283 Measurement of tW production in the semileptonic channel in pp collisions at 13 TeV with CMS

A measurement of the associated production of a single top quark and a W boson in the final states with an electron or muon and jets using pp collisions with $\sqrt{s} = 13$ TeV collected by the CMS detector at the CERN LHC is presented. The data used correspond to an integrated luminosity of 36 fb$^{-1}$ . This result is the first observation of the tW process in the final states containing a muon or electron and jets, with an observed significance clearly exceeding 5 standard deviations. The measured signal strength is μ = 1.24 ± 0.18, consistent with unity. The inclusive cross section is determined to be 89 ± 4 (stat) ± 12 (syst) pb.

Speaker: Duncan Leggat (Chinese Academy of Sciences (CN))

2021-06_lhcp_tWLjets_poster.pdf

Poster video explanation

Zoom meeting room

284 Measurements of differential and integrated fiducial cross sections for Higgs Boson production in the four-lepton decay channel using run 2 data with the CMS detector

After the discovery of the Higgs boson and its characterisation, we are entering in the precision era of the Higgs physics where we need robust measurements to spot any sign of BSM physics. Among the many available tools, fiducial measurements are one of the most used in HEP due to their model independence, longevity, and easy comparison with theoretical predictions. The production cross section is measured by removing detector effects and backgrounds using an unfolding procedure.

Integrated and differential fiducial cross sections for the production of the Higgs boson in pp collision at the LHC at a $\sqrt{s}$=13 TeV via the H$\rightarrow$ZZ$\rightarrow$4$\ell$ ($\ell$=$e$,$\mu$) channel are presented. The dataset was collected by the CMS experiment in 2016, 2017, and 2018, equivalent to a validated integrated luminosity of 137 fb$^{-1}$.

Speaker: Alessandro Tarabini (LLR, École polytechnique (FR))

TarabiniAlessandro_LHCP2021poster.pdf

Video

Zoom meeting room

285 Measurements of inclusive photons and charged particles at forward rapidities in p-Pb collisions at $\sqrt{s\rm_{NN}}$ = 5.02 TeV with ALICE

At high energy collisions, such as those achieved at the LHC, particle production is dominated by soft-QCD processes. The soft production is described by non-perturbative QCD and challenges existing phenomenological models. Global observables such as multiplicity and rapidity dependence of particle production are some of the most fundamental measurements for improving and constraining these models.

In this talk, we will present the multiplicity and pseudorapidity distributions of inclusive photons and charged particles at forward rapidities in p-Pb collisions at $\sqrt{s\rm_{NN}}$ = 5.02 TeV. The Photon Multiplicity Detector measures photon production within 2.3 < $\eta$ < 3.9. The Silicon Pixel Detector and the Forward Multiplicity Detector together measure charged particles over a wide range of -3.4 < $\eta$ < 5.0. Results on centrality evolution of particle production in p-Pb collisions will be presented both for photons and charged particles in comparison with phenomenological models (such as HIJING, DPMJET) based on different initial conditions and particle production mechanisms.

Speaker: Mr Abhi Modak (Bose Institute (IN))

2021-06-10-LHCP_poster_Abhi.pdf

Zoom meeting room

286 Measurements of the inclusive and differential production cross sections of a top-quark–antiquark pair in association with a Z boson at sqrt(s) =13 TeV with the ATLAS detector

An increasing center-of-mass energy of proton-proton collisions and higher luminosities at the CERN Large Hadron Collider make it possible to study rare processes of the Standard Model (SM). In this poster, the measurements of both the inclusive and differential cross sections of top-quark–antiquark production in association with a Z boson (ttZ) are presented. Collision data corresponding to a total integrated luminosity of 139/fb, recorded in years 2015-2018 with the ATLAS detector at a center-of-mass energy of 13 TeV are analysed. Both inclusive and differential measurements are performed by selecting final states with either three or four isolated leptons (electrons or muons). The inclusive cross section is measured to be 0.99 +/- 0.05 (stat.) +/- 0.08 (syst.)~pb, in agreement with the most precise theoretical predictions of the SM. In the differential measurements both absolute and normalised cross sections are measured as a function of a number of kinematic variables which probe the kinematics of the ttZ system. Differential measurements are performed at particle and parton levels for specific fiducial phase-space volumes and are compared with theoretical predictions at different levels of precision. Based on a chi^2/ndf and p-value compatibility comparison, good agreement is observed between the measured differential cross sections and the SM predictions.

Speaker: Dominik Babal (Comenius University (SK))

Poster video explanation

ttZ_LHCP2021.pdf

Zoom meeting room

287 Measurements of the weak diboson production cross sections in leptonic decays at 5.02 TeV with the CMS experiment

We explore a new center-of-mass energy at 5 TeV, to study diboson production in proton-proton collisions using data collected with the CMS detector. The WW, WZ, and ZZ cross sections are measured analyzing events with two, three, or four charged leptons in the final state. These measurements are compared with the best available theoretical predictions and across other experiments.

Speaker: Carlos Vico Villalba (Universidad de Oviedo (ES))

LHCP2021_Dibosons5TeV.pdf

Zoom session

288 Multi-charged TeV scale scalars and fermions in the framework of a radiative seesaw model

Explaining the tiny neutrino masses and non-zero mixings have been one of the key motivations for going beyond the framework of the Standard Model (SM). We discuss a collider testable model for generating neutrino masses and mixings via radiative seesaw mechanism. That the model does not require any additional symmetry to forbid tree-level seesaws makes its collider phenomenology interesting. The model includes multi-charged fermions/scalars at the TeV scale to realize the Weinberg operator at 1-loop level. After deriving the constraints on the model parameters resulting from the neutrino oscillation data as well as from the upper bound on the absolute neutrino mass scale, we discuss the production, decay and resulting collider signatures of these TeV scale fermions/scalars at the Large Hadron Collider (LHC). We consider both Drell-Yan and photo-production. The bounds from the neutrino data indicate the possible presence of a long-lived multi-charged particle (MCP) in this model. We obtain bounds on these long-lived MCP masses from the ATLAS search for abnormally large ionization signature. When the TeV scale fermions/scalars undergo prompt decay, we focus on the 4-lepton final states and obtain bounds from different ATLAS 4-lepton searches. We also propose a 4-lepton event selection criteria designed to enhance the signal to background ratio in the context of this model.

Speaker: Mr Avnish . (Institute of Physics)

Model_Fermion-merged.pdf

Zoom meeting room

289 New ideas on detector technology for the ILC experiments

Detector concepts are being developed for the foreseen electron-positron International Linear Collider (ILC) in Japan. Set to run as a Higgs Factory, ILC will address a rich scientific program from electroweak physics to BSM. The detectors are being optimized for precision physics in a range of energies between 90 GeV and 1 TeV. This poster will summarized the required performance of detectors, the proposed implementation and the readiness of different technologies needed for the deployment at ILC.

Speaker: Mr Bohdan Dudar (DESY)

Poster

Poster video explanation

Zoom meeting room

290 New Small Wheel sTGC Front-End Electronics Integration and Commissioning for ATLAS Phase I Upgrade

The ATLAS Muon Spectrometer is going through an extensive Phase I upgrade to cope up with the future LHC runs of high luminosity of up to 7.5×10$^{34}$ cm$^{-2}$s$^{-1}$. The innermost and first station of the Muon end cap system, the Small Wheel, will be replaced by the New Small Wheel, which has high trigger and precision tracking capabilities. This is achieved by a combination of two detector technologies, Small-Strip Thin Gas Chamber (sTGC) and Micro Mesh Gaseous structures (MM). MM is used for the precision tracking and sTGC is used as a primary trigger detector because of its timing resolution (drift time of most electrons shorter than one bunch crossing period (25 ns) and the front-end ASICs (Application Specific Integrated Circuit), VMMs, can make measurement with precision of 2 ns along with the amplitude measurement). We are working extensively on the integration and commissioning of the front-end electronics for the sTGC chambers. Considering the complexity of the system we are dealing with, we are working to resolve many challenges to test large number of physical channels (~354K) and ASICs (more than 11K) with three different types – pads, strips and wires. We will present our experiences with the trigger and the readout performance studies of the electronics.

Speaker: Prachi Atmasiddha (University of Michigan, Ann Arbor)

LHCP2021_poster_PrachiAtmasiddha.pdf

Zoom meeting room

291 NNLO QCD study of polarised $W^+W^−$ production at the LHC

Longitudinal polarisation of the weak bosons is a direct consequence of Electroweak symmetry breaking mechanism providing an insight into its nature, and is instrumental in searches for physics beyond the Standard Model. We perform a polarisation study of the diboson production in the $pp \to e^+ \nu_e \mu^- \bar\nu_\mu$ process at NNLO QCD in the fiducial setup inspired by experimental measurements at ATLAS. This is the first polarisation study at NNLO. We employ the double pole approximation framework for the polarised calculation, and investigate NNLO effects arising in differential distributions.

Speaker: Andrei Popescu (University of Cambridge)

Popescu_WW-Polarisation-Study_LHCP21.pdf

Poster video introduction

Zoom meeting room

292 Particle-yield modification in jet-like azimuthal V0–hadron correlations in Pb–Pb collisions at 5.02 TeV with ALICE at the LHC

The measurement of azimuthal correlations between two particles is a powerful tool to investigate the properties of strongly-interacting nuclear matter created in ultra-relativistic heavy-ion collisions. In particular, studying the near-side and away-side hadron yields associated with trigger particles can provide important information to understand both the jet -medium interaction and hadron production mechanism. We study two-particle correlations with V0 (K0s, Λ/Λ ) and charge hadrons as trigger particles of transverse momentum 8 < pT,trig < 16 GeV/c,and associated charged particles of 1 GeV/c < pT,assoc < pT,trig at mid-rapidity in pp and Pb–Pb collisions at a center-of-mass energy of 5.02 TeV per nucleon pair. After subtracting the contributions of the flow background v2 and v3 , the per-trigger yields are extracted for two-particle azimuthal differences |∆φ| < 0.9 on the near-side and |∆φ − π| < 1.2 on the away-side.
The ratio of the per-trigger yields in Pb–Pb collisions with respect to pp collisions , IAA, is measured in the near-side and away-side in the most central 0–10% collisions. On the near-side,a significant enhancement of IAA from 1.5 to 2 for different particles species is observed at the lowest pT,assoc. On the away-side, suppression to the level of (I AA ≈ 0.6 ) for pT,assoc>3 GeV/c is observed as expected from strong in-medium energy loss while an enhancement reaching 1.4
at the lowest pT,assoc . The data are compared to AMPT, HIJING and EPOS models. Most calculations qualitatively describe the near-side and away-side yield modification at intermediate and high pT,assoc .

Speaker: Mustafa Anaam (Central China Normal University CCNU (CN))

Particle yield modification LHCP poster.pdf

293 Performance monitoring of the GE1/1 Triple-GEM detectors for the CMS Muon System

The muon system of the CMS experiment has been instrumented with two wheels of triple-GEM detectors in order to ensure redundancy in the pseudo-rapidity region 1.55-2.2 so keeping the trigger rate at an acceptable level while not compromising the CMS physics potential in Run 3 of the LHC. The station, named GE1/1, provides two additional muon hit measurements which will improve the muon tracking and triggering performance in combination with the existing CSC detectors. As the commissioning phase of the detector is ongoing, prompt assessment of the muon detection performance is crucial for adjusting the operating parameters of the detector and its electronics. This contribution will present a set of analysis tools developed for the detector performance monitoring based on tools common to all the CMS muon subdetectors. Validation of the analysis based on simulations will be discussed, together with preliminary results obtained from cosmic-ray events.

Speaker: Gabriele Milella (Universita e INFN, Bari (IT))

MilellaSimone_LHCP2021_performance_monitoring_GEM_poster_v1.pdf

Zoom meeting room

294 Performance of the Tile Calorimeter Demonstrator system for the ATLAS Phase-II Upgrade

The High Luminosity Large Hadron Collider (HL-LHC) will deliver five times the LHC nominal instantaneous luminosity, after a series of upgrades that will take place during the shutdown of 2024 –2026. The ATLAS Hadronic Calorimeter (TileCal) will require the complete replacement of the readout electronics in order to accommodate its acquisition system to the increased radiation levels, trigger rates, and high pile-up conditions during the HL-LHC era.The upgraded readout electronics will digitize the PMT signals from every TileCal cell for every bunch crossing and will transmit them directly to the off-detector electronics. In the counting rooms, the off-detector electronics will store the calorimeter signals in pipelined buffers while transmitting reconstructed trigger objects to the first level of trigger at 40 MHz.The TileCal upgrade project has undergone an extensive R&D program and several test beam campaigns. A Demonstrator module has been assembled using the upgraded on-detector electronics and tested in the ATLAS experiment. The Demonstrator module is operated and read out using a prototype of Tile PreProcessor (TilePPr) which also permits integrating the Demonstrator module into the present ATLAS TDAQ system. This contribution presents the status and performance of the Demonstrator module in the ATLAS experiment.

Speaker: Edward Khomotso Nkadimeng (University of the Witwatersrand (ZA))

Performance of the TileCal Demonstator System for the ATLAS Phase-II Upgrade LHCP 2021.pdf

Poster Explaination Tile Demonstrator system for the ATLAS Phase-II Upgrade.mp4

Poster Landscape Performance of Tile Demonstrator system for the ATLAS Phase-II Upgrade.pdf

ZOOM poster room

295 Physics motivations and detector upgrades for the new era of the ATLAS experiment

With the end of RUN-II, the LHC has delivered only 4% of the collision data expected to be available during its lifetime. The next data-taking campaign - RUN-III - will double the integrated luminosity the LHC accumulated in 10 years of operation. The Run-III will be the herald of the HL-LHC era, an era when 90% of total LHC integrated luminosity (4 ab$^{-1}$) will be accumulated allowing ATLAS to perform several precision measurements to constrain the Standard Model Theory (SM) in yet unexplored phase-spaces and in particular in the Higgs sector, only accessible at LHC. Direct searches have so far provided no indication of new physics beyond the Standard Model, however, they can be complemented by indirect searches that allow extending the reach at higher scales. Indirect searches are based on the ability to perform very precise measurements, a highly complex task at a hadron collider that will require tight control of theoretical predictions, reconstruction techniques, and detector operation. Moreover, populating extreme regions of phase-space for multi-differential production cross-section analysis will require the development and validation of Monte Carlo phase-space biasing techniques and efficient integration methods to produce the billions of events needed to cope with higher luminosities.
To answer the quest for high precision measurements in a high luminosity environment, a comprehensive upgrade of the detector and associated systems was devised and planned to be carried out in two phases. The Phase-I upgrade program foresees new features for the muon detector, for the electromagnetic calorimeter trigger system, and for all trigger and data acquisition chain and will operate to accumulate about 350 fb$^{-1}$ of integrated luminosity during the RUN-III. The RUN-III will mark the debut of a new trigger system designed to cope with more than 80 simultaneous collisions per bunch crossing. After this, ATLAS will proceed with the Phase-II upgrade to prepare for the high luminosity frontier where the ATLAS experiment will face more than 200 simultaneous collisions per bunch crossing and a high radiation level for many sub-systems. The Phase-II upgrade comprises a completely new all-silicon tracker with extended rapidity coverage that will replace the current inner tracker detector; the calorimeters and muon systems will have their trigger and data acquisition systems fully redesigned, allowing the implementation of a free-running readout system. Finally, a new subsystem called High Granularity Timing Detector will aid the track-vertex association in the forward region by incorporating timing information into the reconstructed tracks. A final ingredient, relevant to almost all measurements, is a precise determination of the delivered luminosity with systematic uncertainties below the percent level. This challenging task will be achieved by collecting the information from several detector systems using different and complementary techniques.
The presentation will focus on physics goals within the reach of Run-III and on the status of ongoing detector upgrades. An outlook toward the HL-LHC challenges will also be presented.

Speaker: Marisilvia Donadelli (Universidade de Sao Paulo (BR))

ATL-COM-UPGRADE-2021-021.pdf

Zoom meeting room

296 Physics Potential and Track Reconstruction of the FASER Experiment

FASER (ForwArd Search ExpeRiment) is a new, small and inexpensive experiment designed to search for light, weakly interacting particles during Run 3 of the LHC. Such particles may be produced in large quantities in proton-proton collisions, travel for hundreds of meters along the beam axis, and can decay in two charged Standard Model particles. To reach its physics goals, a good hit resolution, and track reconstruction to separate the two closely-spaced, oppositely charged tracks is essential. In this poster, I review the physics discovery potential of FASER and the status of the track reconstruction, which is based on the ACTS toolkit. ACTS aims to provide an experiment-independent toolkit for track reconstruction.

Speaker: Mr Tobias Boeckh (University of Bonn (DE))

LHCP2021_Physics-potential-and-track-reconstruction-of-the-FASER-experiment.pdf

poster-video-explanation.mp4

Zoom meeting room

297 Playing cards as a tool to create public interest in physics

A novel outreach project is presented that makes use of playing cards – one of the most ubiquitous toys around the world – to communicate physics in a fun, engaging manner. A custom deck of cards has been designed to inspire an interest in physics while being widely appealing to the general public and useful for gameplay, magic and cardistry. In the course of bringing this project to completion, many different social media platforms and channels are explored and used to facilitate communication about the project and physics in general. The project has presented opportunities for unusual collaborations. The cards will soon be in production and have excellent potential for use in outreach events and educational settings.

Speaker: Jason Robert Veatch (Georg August Universitaet Goettingen (DE))

LHCP2021_jveatch.pdf

Zoom meeting room

298 Possibility of Total Ionizing Dose Effects measurements for LHC experiments elements in a medical facility: the TIFPA-INFN experience

Total Ionizing Dose Effects tests and measurements are crucial requirements for solid state particle sensors and electronic control systems qualification in all the LHC present experiments and future upgrades.
These measurements can be performed not only in facilities explicitly built for this mission, but with some wisdom, also in medical or biological research facilities when some minimum requirements are present. In this poster will be shown the pianification and realization of SiPM x-ray irradiations for TID measurements realized in the italian TIFPA-INFN Trento Center laboratory.
In detail will be described the minimum flexibility required by the x-ray irradiation set-up, by the dose measurement system, the irradiation pianification and realization.
Finally will be presented the limitations observed in these measurements, how can be minimized and the final results.

Speaker: Dr Benedetto Di Ruzza (INFN - National Institute for Nuclear Physics (Italy))

BenedettoDiRuzza_LHCP2021_poster.pdf

BenedettoDiRuzza_LHCP2021_slides.pdf

Zoom Poster Room

299 Precision from Diboson Processes at FCC-hh

Thanks to its high luminosity and center of mass energy, the future FCC-hh collider will allow us to probe processes with clean but rare final states that are unaccessible at the LHC. The study of diboson production processes poses a promising way of indirectly constraining New Physics in the context of the Higgs Boson. Specifically, the diphoton leptonic decay channels of the Wh and Zh production processes are examples for the aforementioned clean but rare final states. I will discuss our study of these channels at the FCC-hh in the SMEFT framework and how doubly differential distributions can be used to gain even better sensitivity to certain higher dimensional EFT operators.

Speaker: Philipp Englert (DESY Hamburg)

LHCP2021_Englert.pdf

ZOOM poster room

300 Precision Luminosity Measurement with the CMS detector at HL-LHC

The high-luminosity upgrade of the LHC (HL-LHC) is foreseen to reach an instantaneous luminosity a factor of five to seven times the nominal LHC design value. The resulting, unprecedented requirements for background monitoring and luminosity measurement create the need for new high-precision instrumentation at CMS, using radiation-hard detector technologies. This contribution presents the strategy for bunch-by-bunch online luminosity measurement based on various detector technologies. A main component of the system is the Tracker Endcap Pixel Detector with dedicated triggers for online measurement of luminosity and beam-induced background using pixel cluster counting on an FPGA. The potential of the exploitation of the outer tracker, the hadron forward calorimeter and muon trigger objects is also discussed, as well as the concept of a standalone luminosity and beam-induced background monitor using Si-pad sensors.

Speaker: Cristina Oropeza Barrera (Universidad Iberoamericana (MX))

Luminosity-CMS_HL-LHC_Oropeza-Barrera.pdf

Zoom meeting room

301 Precision Timing with the CMS MTD Barrel Timing Layer for HL-LHC

The Compact Muon Solenoid (CMS) detector at the CERN Large Hadron Collider (LHC) is undergoing an extensive Phase II upgrade program to prepare for the challenging conditions of the High-Luminosity LHC (HL-LHC). A new timing detector in CMS will measure minimum ionizing particles (MIPs) with a time resolution of 30-40 ps for MIP signals at a rate of 2.5 Mhit/s per channel at the beginning of HL-LHC operation. The precision time information from this MIP Timing Detector (MTD) will reduce the effects of the high levels of pileup expected at the HL-LHC, bringing new capabilities to the CMS detector. The barrel timing layer (BTL) of the MTD will use sensors that are based on LYSO:Ce scintillation crystals coupled to SiPMs with TOFHIR ASICs for the front-end readout. In this talk we will present motivations for precision timing at the HL-LHC and an overview of the MTD BTL design, including ongoing R&D studies targeting enhanced timing performance and radiation tolerance.

Speaker: Badder Marzocchi (Northeastern University (US))

LHCP_MTD_Poster_Badder_Marzocchi.pdf

Zoom meeting room

302 Projections for jet quenching measurements in O-O collisions at $\sqrt{s_{NN}}$= 6.37 TeV during the LHC Run3

High-multiplicity events in small collision systems (pp, p-Pb) at LHC energies exhibit soft-physics phenomena that are associated with collective dynamics of the quark-gluon plasma (QGP) in large collision systems, e.g. azimuthal correlation between soft particles having large pseudo-rapidity separation. Jet quenching is likewise a necessary consequence of the formation of a QGP. However, within the precision of current measurements there is no significant evidence of jet quenching in small systems. Improvement of the experimental sensitivity to jet quenching in small collisions systems is therefore essential to address the question of the limits of QGP formation.

In Run3, the LHC will carry out a brief run with O-O collisions at $\sqrt{s_{NN}}$ = 6.37 TeV. The O-O system bridges the gap in system size between pp and p-Pb on one side and Pb-Pb on the other, and provides measurement channels in which quenching effects are expected to be both observable experimentally and calculable theoretically. The poster will present projections for high-precision measurements of jet quenching in the O-O run by ALICE.

Speaker: Filip Krizek (Czech Academy of Sciences (CZ))

KrizekFilip_LHCp21_poster_v1.pdf

Zoom meeting room

303 Prospects to exclude top quark partners using full Run II, III and HL-LHC data sets

This talk discusses the prospects under various scenarios of the amount of data collected and assumptions on systematic uncertainties to explore the top squark and neutralino mass degenerate corridor. The analysis technique employs a deep neural network fed with variables sensitive to top quark spin correlation and polarization in top quark pair production. In particular, different improvements on experimental and theoretical uncertainties are studied in terms of their impact on sensitivity as well as the amount of data collected, e.g. proton-proton collisions at the LHC collected during Run II, upcoming Run III and the HL-LHC. Further improvements of the method and sensitivity are possible by a multi-differential measurements of the full spin density production matrix and other angular observables of top quarks pairs and we highlight the impact and plans of these.

Speaker: Amandeep Singh Bakshi (Purdue University)

LHCP_2021_poster.pdf

Zoom meeting room

304 Pseudo-gauge dependence of quantum fluctuations of energy in a hot relativistic fermionic gas

Explicit expressions for quantum fluctuations of energy in subsystems of a hot relativistic gas of spin-1/21/2 particles are derived. The results depend on the form of the energy-momentum tensor used in the calculations, which is a feature described as pseudo-gauge dependence. However, for sufficiently large subsystems the results obtained in different pseudo-gauges converge and agree with the canonical-ensemble formula known from statistical physics. As different forms of the energy-momentum tensor of a gas are a priori equivalent, our finding suggests that the concept of quantum fluctuations of energy in very small thermodynamic systems is pseudo-gauge dependent. On the practical side, the results of our calculations determine a scale of coarse graining for which the choice of the pseudo-gauge becomes irrelevant.

Speaker: Mr Rajeev Singh (Institute of Nuclear Physics Polish Academy of Sciences)

LHCP2021-Rajeev.pdf

LHCP2021_Rajeev_Singh.pdf

Pseudo-gauge dependence of quantum fluctuations of energy in a hot relativistic gas of fermions

Zoom room (password: 20210610)

305 Real-time flavour tagging selection in ATLAS

In high-energy physics experiments, online selection is crucial to select interesting collisions from the large data volume. ATLAS b-jet triggers are designed to identify heavy-flavour content in real-time and provide the only option to efficiently record events with fully hadronic final states containing b-jets. In doing so, two different, but related, challenges are faced. The physics goal is to optimise as far as possible the rejection of light jets, while retaining a high efficiency on selecting b-jets and maintaining affordable trigger rates without raising jet energy thresholds. This maps into a challenging computing task, as tracks and their corresponding vertexes must be reconstructed and analysed for each jet above the desired threshold, regardless of the increasingly harsh pile-up conditions. We present an overview of the ATLAS strategy for online b-jet selection for the LHC Run 2, including the use of novel methods and sophisticated algorithms designed to face the above mentioned challenges. The evolution of the performance of b-jet triggers in Run 2 data is presented, including the use of novel triggers designed to select events containing b-jets in heavy ion collisions.

Speaker: Christian Nass (University of Bonn (DE))

Poster_landscape_wPaperPlots.pdf

Zoom meeting room

306 Renormalization of scalar EFTs at higher orders

Because of its ability to systematically capture beyond Standard Model (SM) effects, effective field theory (EFT) has received much attention in phenomenological analyses of e.g. LHC data. Recent theoretical studies have focused on operator basis construction and loop level calculations in EFTs. In this work, we construct the complete basis for scalar $\phi^4$ EFT up to mass dimension 12, with the help of the Hilbert series method. We present high loop calculations (up to 5 loop), and find unexpected zeros and interesting symmetric structures in the anomalous dimension matrix. The method we use can be extended to more general theories, i.e. SMEFT and be applied in high precision measurements within the SMEFT framework at the LHC.

Speaker: Weiguang Cao (Kavli IPMU)

poster_Renormalization of scalar EFTs at higher orders.pdf

Zoom Meeting Room

307 Search for charged Higgs bosons decaying to W+W+ or W+Z in 139fb-1 of sqrt(s)=13TeV pp collisions with the ATLAS detector

This poster presents a search for charged Higgs bosons decaying into 𝑊𝑊 or 𝑊𝑍 bosons, involving experimental signatures with two leptons of the same charge, or three or four leptons with a variety of charge combinations, missing transverse momentum and jets. Some focus will be given on the four leptons channel signature. A data sample of proton–proton collisions at a centre-of-mass energy of 13 TeV recorded with the ATLAS detector at the Large Hadron Collider between 2015 and 2018 is used. The data correspond to a total integrated luminosity of 139 fb−1. The search is guided by a type-II seesaw model that extends the scalar sector of the Standard Model with a scalar triplet, leading to a phenomenology that includes doubly and singly charged Higgs bosons. Two scenarios are explored, corresponding to the pair production of doubly charged 𝐻 bosons, or the associated production of a doubly charged 𝐻 boson and a singly charged 𝐻 boson. No significant deviations from the Standard Model predictions are observed. 𝐻 bosons are excluded at 95% confidence level up to masses of 350 GeV and 230 GeV for the pair and associated production modes, respectively.

Speaker: Iulia-Stefania Trandafir (Horia Hulubei National Institute of Physics and Nuclear Engineering)

Poster-LHCP2021-Iulia_TRANDAFIR.pdf

Slides-LHCP2021-Iulia_TRANDAFIR.pdf

Zoom meeting room

308 Search for Dark Matter produced in association with a Standard Model Higgs boson decaying to b-quarks with 139 fb−1 of pp collision data with the ATLAS detector

Many extensions of the Standard Model predict the production of Dark Matter in association with Higgs bosons.
This search examines the final state of missing transverse momentum
accompanied by a bb pair coming from a Higgs boson decay. For this purpose proton-proton
collision data is used which is produced at 13 TeV centre-of-mass energy and recorded by the
ATLAS experiment at the LHC, amounting to an integrated luminosity of 139 fb−1.
The increase in integrated luminosity in conjunction with many analysis optimizations result in
a better sensitivity in comparison to previous iterations. No significant deviation from the
Standard Model is observed and the results are interpreted in the context of the 2-Higgs
doublet models with an additional vector or pseudoscalar mediator.

Speaker: Janik Von Ahnen (Deutsches Elektronen-Synchrotron (DE))

2021_LHCP_JanikVonAhnen_MonoHbbMET.pdf

Zoom meeting room

309 Search for electroweak production of charginos and neutralinos in final states with one lepton, jets and missing transverse momentum with the ATLAS experiment

This poster presents a search for electroweak production of mass degenerate chargino-neutralino pairs in the context of R-parity conserving supersymmetric simplified models in which the chargino decays into W boson and the lightest neutralino, while the next-to-lightest neutralino decays into either Higgs or Z boson, in addition to the lightest neutralino. This search concentrates on final states characterized by the presence of one isolated charged lepton (either electron or muon) accompanied by jets and missing transverse momentum. The analysis exploits an integrated luminosity of 139 fb-1 which corresponds to the full Run-2 of proton-proton collisions data recorded by the ATLAS detector at Large Hadron Collider. No statistically significant evidence of a deviation from the Standard Model expectation is observed. Expected and observed 95% C.L limits are set based on the chargino and the lightest neutralino mass, assuming pure wino production cross-sections.

Speaker: Ngoc Khanh Vu (Centre National de la Recherche Scientifique (FR))

LHCP2021_Poster_NgocKhanhVU.pdf

Poster video explantion

Zoom meeting room

310 Search for exotic decays of the Higgs boson to long-lived particles using displaced vertices in the ATLAS inner detector

A novel search for exotic decays of the Higgs boson to pairs of long-lived
neutral particles, each decaying to a bottom quark pair, is performed
using 139 fb$^{-1}$ of $\sqrt{s} = 13$ TeV proton-proton collision data
collected with the ATLAS detector at the LHC. Events consistent with the
production of a Higgs boson in association with a $Z$ boson are analyzed,
with the leptonic decay of the $Z$ mitigating the trigger challenges associated
with displaced objects. Long-lived particle (LLP) decays are reconstructed from
inner detector tracks as displaced vertices with high mass and track multiplicity
relative to Standard Model processes. The analysis selection requires the
presence of at least two displaced vertices, effectively suppressing Standard Model
backgrounds. The residual background contribution is estimated using a fully data
driven technique. No excess over the Standard Model prediction is observed, and
upper limits are set on the branching ratio of the Higgs boson to pairs of LLPs.
Branching ratios of >=10% are excluded at the 95% confidence level for
LLP mean proper lifetimes $c\tau$ as small as 4 mm and as large as 110 mm.
For LLP masses below 40 GeV, these results represent the most stringent
constraints to date for this range of proper lifetimes.

Speaker: Jackson Carl Burzynski (University of Massachusetts (US))

LHCP2021.pdf

Zoom meeting room

311 Search for heavy resonances decaying into a W boson and a Higgs boson in lvbb final states in 139fb-1 of root(s)=13TeV pp collisions with the ATLAS detector

This poster presents the search for new resonances decaying into a W boson and a 125GeV Higgs boson in the lvbb final state, where l=e+- or mu+-, in pp collisions at root(s)=13TeV. The search includes a channel requiring one lepton and missing transverse energy, as well as a channel with only missing transverse energy for the case where the lepton is not reconstructed. The data used correspond to a total integrated luminosity of 139fb-1 collected with the ATLAS detector at the Large Hadron Collider with the full Run-2 dataset. The search is conducted by examining the reconstructed invariant and transverse mass distributions of Wh candidates for evidence of a localized excess in the mass range of 400GeV up to 5TeV. Upper limits are placed at the 95% confidence level on the production cross-section times branching fraction of heavy W' resonances in heavy-vector-triplet models.

Speaker: Makayla Vessella (University of Massachusetts (US))

LHCP2021Wprime.pdf

Zoom meeting room

312 Search for H→ ccbar at a Multi-TeV Muon Collider

A Multi-TeV (√s=1.5-10TeV) muon collider providing O(1/ab)integrated luminosity will be a great opportunity to probe the most intimate nature of the Standard Model (SM) and the Electroweak Symmetry Breaking mechanism, allowing the precise measurement of the Higgs couplings to several SM particles. The study of the Higgs boson couplings to the second generations of fermions is of particular interest due to sensitivity to a whole class of new physics models. On the other end, this measurement is extremely challenging, because of the small branching ratio. We explored, for the first time, the search for H→ccbar at a multi-TeV muon collider. The μ+μ− →Hνν¯→ cc¯νν¯ signal process has been fully simulated and reconstructed with a preliminary detector design, along with the main backgrounds. A c quark-tagging algorithm has been developed, combining several observables in a single discriminator using Machine Learning techniques, with the goal to improve the rejection of jets coming from b-quark and u-d-s-g hadronization. A first estimate of the precision on the Higgs coupling with c-quark reachable with a muon collider machine will be presented.

Speaker: Paola J Mastrapasqua (Universita e INFN, Bari (IT))

Poster video explanation

Search_for_Hcc_Paola_Mastrapasqua.pdf

Zoom meeting room

313 Search for H→ ZZ*→ 4µ at a Multi-TeV Muon Collider

A muon collider represents the ideal machine to reach very high center-of-mass energies (√s=1.5-10TeV) and luminosities O(0.5-10/ab). A large number of Higgs bosons will be produced mainly through the Vector Boson Fusion (VBF) processes. The VBF through Z bosons (ZZH) production process could be difficult to disentangle to the dominant WWZ, since the final state VBF muons, produced in the very forward region, could escape the detector. As a consequence, the H→ ZZ decay process turns out to be favoured to probe exclusively the Higgs bosons coupling with Z bosons at a multi-TeV muon collider. In addition, a feasibility study of H→ ZZ search in such an environment is mandatory before assessing the feasibility of more appealing measurements such as the trilinear and quartic Higgs boson coupling.
We will present, for the first time, a feasibility study of the H→ ZZ* → 4µ process in a multi-TeV muon collider. The study of the 4 muons final state, performed on fully simulated Monte Carlo samples, allows to optimize the muon reconstruction, thus providing feedback for the detector design. Reducible background induced by the muons decaying in the beam pipe and irreducible backgrounds from Standard Model have been studied, together with dedicated Machine Learning techniques for their reduction. A first estimate on the Higgs coupling to Z bosons in the 4µ channel will be provided.

Speaker: Angela Zaza (Universita e INFN, Bari (IT))

HZZ_4mu_MuonCollider_AngelaZaza.pdf

Poster video explanation

Zoom meeting room

314 Search for jet quenching effects in high-multiplicity proton-proton collisions at $\sqrt{s} = 13~\rm{TeV}$

Small collision systems, such as pp or p-Pb, exhibit signatures of collective effects that are thought to be associated with quark-gluon plasma formation. The absence to date of jet quenching signals raises a question about the origin of the observed collectivity and calls for more accurate jet quenching measurements in small collision systems. In this poster, the ALICE Collaboration reports results of a novel approach to search for jet quenching effects in high-multiplicity pp collisions at $\sqrt{s}$ = 13 TeV, which are selected based on charged-particle multiplicity measured using forward scintillator detectors. In the analysis, we look for broadening of the azimuthal acoplanarity measured by the semi-inclusive distribution of charged-jets recoiling from a high transverse momentum, charged trigger hadron. Jet reconstruction is performed using anti-$k_{\rm {T}}$ algorithm with $R$ = 0.4. The measured jet yield is corrected for uncorrelated background,including multi-partonic interaction, by means of a data-driven statistical method. Comparison of recoil jet distributions measured in minimum bias and high-multiplicity events reveals significant broadening in the high-multiplicity data, resembling jet quenching. However, a qualitatively similar feature is observed in pp data simulated with the PYTHIA 8 generator, which does not account for jet quenching. We will discuss the current status of the analysis, and prospects to understand the origin of this striking phenomenon.

Speaker: Artem Kotliarov (Czech Academy of Sciences (CZ))

LHCP2021_Poster_Kotliarov.pdf

Zoom meeting room

315 Search for New Heavy Neutral Gauge Boson using Vector Boson Fusion Processes at the LHC

To address the incompleteness of the Standard Model (SM), many models introduce new gauge fields and interactions, which manifest as new particles with TeV scale masses. Thus, it is imperative to understand particles and interactions at the TeV scale. An example of one such particle is the $Z^\prime$ boson, a heavy, neutral spin-1 gauge boson. Numerous ideas exist to probe the TeV scale, motivating a large volume of $Z^\prime$ searches at the LHC. However, those searches have failed to show signs of new physics. Possible explanations point to new physics having different features to what is traditionally assumed in $Z^\prime$ searches, remaining concealed in processes not yet investigated. In particular, existing searches targeting Drell-Yan processes rely on a sizable coupling for the $Z^\prime$ to light quarks ($g_{\ell}$). This talk focuses on a search for $Z^\prime$ produced via vector boson fusion processes (VBF), whose production rate is independent of $g_{\ell}$, and which has non-universal fermion couplings (NUFC). Scenarios with NUFC are motivated by the recent anomalies in the $B$-physics sector and the muon anomalous magnetic moment.

Speaker: Ms Amandeep Kaur (Panjab University (IN))

VBFZprime_LHCP2021Poster_FINAL.pdf

VBFZprime_LHCP2021Poster_slides.pdf

Zoom meeting room

316 Search for New Resonance in Photon and Jet final State using CMS Data

Several theoretical models of Beyond the Standard Model (BSM) physics predicts the production of new resonances at hadron collider experiments. This study, in particular, is focused on the search for Quantum Black hole (QBH) and existence of substructure of light and heavy flavor quarks in the photon + jet final state in the proton-proton collisions at a centre of mass energy of 13 TeV using the data collected by the CMS detector in the LHC Run-2 period. The exclusion limits are set on the model parameters in the absence of a signal in the data.

Speaker: Ms Jyoti Babbar (Panjab University (IN))

LHCP_final.pdf

LHCP_poster.pdf

Zoom meeting room

317 Search for non-resonant di-Higgs production in the HH->bbyy decay channel in pp collisions at sqrt(s) = 13 TeV with the ATLAS detector

We present a search for non-resonant di-Higgs production in the HH->bbyy decay channel. The measurement uses 139ifb of pp collisions recorded by the ATLAS experiment at a center-of-mass energy of 13 TeV. Selected events are separated into multiple regions, targeting both the SM signal and BSM signals with modified Higgs self-couplings. No excess with respect to background expectations are found and upper limits at 95% confidence level are set on the di-Higgs production cross sections and the Higgs trilinear coupling modifier.

Speaker: Alex Zeng Wang (University of Wisconsin Madison (US))

conference_poster_2.pdf

Zoom meeting room

318 Search for nonresonant Higgs boson pair production in final states with a pair of b-quarks and a pair of photons in sqrt(s) =13 TeV pp collisions data at CMS experiment

The trilninear self-coupling of Higgs can directly be accessed at the LHC by inclusive production of Higgs pair. A search for the non-resonant Higgs pair production via gluon-gluon fusion (ggF) and as well as Vector Boson Fusion (VBF) processes has been performed recently by CMS collaboration with the complete LHC Run-2 proton-proton collision data at center of mass energy of $\sqrt{s}$=13 TeV, in the most sensitive 2$\gamma$ + 2b jets inclusive final state. This presentation emphasizes on the results of the production cross section of inclusive diHiggs production as well as estimates of relevant coupling parameters.

Speaker: Soumya Mukherjee (Tata Inst. of Fundamental Research (IN))

LHCP_2021_POSTER_HHBBGG.mp4

LHCP-2021_POSTER_HHBBGG_SOUMYA.pdf

LHCP_2021_POSTER_slides.pdf

Zoom meeting room

319 Search for scalar top quark pair production in the top corridor region at the CMS experiment

A search for scalar top quark pair production at the LHC with the CMS experiment is presented. This search targets a region of parameter space where the kinematics of top squark pair production and top quark pair production are very similar because of the mass difference between the top squark and the neutralino being close to the top quark mass. The search is performed with the full run 2 data set of proton-proton collisions at a centre-of-mass energy of 13 TeV, collected by the CMS detector, using events containing dilepton pairs with opposite charge. A DNN algorithm is used to separate signal from background.

Speaker: Andrea Trapote Fernandez (Universidad de Oviedo (ES))

LHCP2021.pdf

Zoom meeting room

320 Search for the dark boson through exotic Higgs decays

A study of long-lived dark Z boson that either couples directly to quarks or mixes kinetically with the standard model Z boson is performed. Production via a vector portal and the Higgs portal are considered. The impact of additionally mixing the standard model Higgs boson with a dark Higgs boson on the production and decays of the dark Z is evaluated. Specifically, decays with a final state of displaced dimuons are considered where the dark Z and the dark Higgs decay directly to a dimuon or indirectly via dark scalars or fermions to an even number of dimuons, which can give rise to final states with large muon multiplicities. The production and total cross sections of the processes of interest as well as decay widths and decay lengths are calculated by applying Monte Carlo simulation using the framework of MadGraph5_aMC@NLO v2.7.0. The sensitivity for such searches in Runs 2 and 3 of the Large Hadron Collider is discussed. Kinematics of the displaced dimuons is also investigated.

Speaker: Tamer Elkafrawy (Florida Institute of Technology (US))

Tamer_Elkafrawy_LHCP2021_v2.pdf

Zoom meeting room

321 Search for W' bosons decaying to a top and a bottom quark at sqrt(s)=13 TeV in the hadronic final state with CMS

A search is performed for W' bosons decaying to a top and a bottom quark in the all-hadronic final state, in proton-proton collisions at a center-of-mass energy of 13 TeV using the data collected by the CMS experiment between 2016 and 2018, corresponding to an integrated luminosity of 137 fb$^{-1}$. Deep neural network algorithms are used to identify the jet initiated by the bottom quark and the jet containing the decay products of the top quark when the W boson from the top quark decays hadronically. No excess above the estimated standard model background is observed. Both left- and right-handed W' bosons with masses below 3.4 TeV are excluded at 95% confidence level, and the most stringent limits to date on W' bosons decaying to a top and a bottom quark in the all-hadronic final state are obtained.

Speaker: Suman Chatterjee (Austrian Academy of Sciences (AT))

Explanation_Suman_Wprime.mp4

https://cern.zoom.us/j/64631032639

LHCP2021_Poster.pdf

LHCP2021_Poster_slides.pdf

322 Sp(4) SIMP Dark Matter on the Lattice

The Strongly Interacting Massive Particle (SIMP) paradigm has recently been increasingly studied. It provides dark matter candidates as pseudo-Goldstone bound states of dark fermions under a new gauge group. In this scenario freezeout occurs through $3\to 2$ dark matter self-annihilation and points to DM particles with masses of $\mathcal O(100 ~\text{MeV})$. We study the spectrum of the lightest mesons of $Sp(4)$ gauge theory with 2 massive almost-degenerate fundamental Dirac fermions using lattice gauge theory. This setup leads to a total of 5 pseudo-Goldstone bosons which can self-annihilate. In particular, we investigate the breaking of the flavour symmetry when making the fermions non-degenerate. We report that one pseudo-Goldstone is lighter than the others while the remaining heavier four pseudo-Goldstones are still mass-degenerate.

Speaker: Fabian Zierler (University of Graz)

LHCP2021_SIMP_DM.pdf

Poster video explanation (vimeo)

Zoom meeting room

323 Spectator nucleons in ultracentral $^{208}$Pb–$^{208}$Pb collisions as a probe of nuclear periphery

As known, nuclear periphery in heavy nuclei is enriched by neutrons. Neutron-to-proton ratio is especially high in a very thin (<0.5 fm) surface layer of such nuclei termed neutron skin (NS). The difference between RMS radii of neutron and proton density distributions is also subtle and difficult to measure. The results obtained with different theoretical and experimental methods are characterized by large uncertainties and sometimes contradict each other. In this work we propose a new method to constrain the parameters of neutron skin by investigating the composition of spectator matter in ultracentral collisions of heavy relativistic nuclei. The yields of spectator neutrons and protons in ultracentral $^{208}$Pb–$^{208}$Pb collisions at the CERN SPS and LHC were calculated within a new version of Abrasion-Ablation Monte Carlo for Colliders model (AAMCC-MST) with accounting for preequilibrium break-up of spectator matter (prefragment) due to its irregular half-moon shape. AAMCC-MST modeling of each collision event was proceeded in several stages. Firstly, the size and shape of spectator prefragments from both colliding nuclei were defined using Glauber Monte Carlo model. Secondly, the excitation energy of the prefragments was calculated. Thirdly, the minimum spanning tree (MST) clustering algorithm was applied to both prefragments to define secondary clusters with their excitation energy estimated depending of their size. Finally, cluster decays were simulated with Fermi Break-up model from Geant4 toolkit. It is found that the simulations of ultracentral $^{208}$Pb–$^{208}$Pb collisions with accounting for NS demonstrate a modest 10% increase of the cross sections to produce a given number of spectator neutrons in comparison to calculations without NS. Similar cross sections, but calculated for events without spectator protons, demonstrate a prominent increase up to 50% due to accounting for NS. The impact of NS on the events with given numbers of spectator protons (N$_{p}$=1,2,3) is also investigated. The dependence of the considered cross sections on the parameters of density distributions of neutrons and protons in $^{208}$Pb has been studied. The considered effects of NS can be studied at the ALICE experiment at the LHC providing that the measurements of neutron and proton yields are properly corrected for the acceptance and efficiency of forward hadronic calorimeters.

Speaker: Nikita Kozyrev (Moscow Institute of Physics and Technology)

LHCP2021_Kozyrev_final.pdf

Poster video explanation

ZOOM poster room

324 Spectral Clustering for Jet Physics

Machine learning (ML) is pushing through boundaries in computational physics.
Jet physics, with it's large and detailed dataset, is particularly well suited.
In this poster I will present work done in https://arxiv.org/abs/2104.01972 on
the application of an unusual ML technique, Spectral Clustering, to jet formation.

Spectral clustering differs from much of ML as it has no "black-box" elements.
Instead, it is based on a simple, elegant algebraic manipulation.
This allows us to inspect the way the algorithm is interpreting the data, and apply physical intuition.

Infrared-collinear (IRC) safety is of critical importance to jet physics.
IRC safety requires that jets formed are insensitive to collinear splitting and soft emissions.
Spectral clustering is shown to be possible to apply in an IRC safe way, and the conditions for this are noted.

Finally, the capacity of spectral clustering to handle different datasets is shown.
Its excellent performance, both in terms of multiplicity and mass peaks is demonstrated.
The reasons for its flexibility are discussed, and potential developments offered.

Speaker: Henry Day-Hall (University of Southampton)

Spectral_poster.pdf

Zoom meeting room

325 Strange-hadron correlation studies to investigate strangeness enhancement in pp collisions

The production of strange and multi-strange hadrons in heavy-ion collisions is enhanced with respect to minimum bias pp collisions. This feature has been further investigated by studying pp collisions as a function of the produced charged particle multiplicity. In pp collisions, the strange hadron yields normalised to the pion yield show an increase with the multiplicity of produced particles. The origin of this striking phenomenon remains an open question: is it related to soft particle production or to hard scattering events, such as jets?

The ALICE experiment has further studied this feature by separating strange hadrons produced in jets from those produced in soft processes. For this purpose, the angular correlation between high-${p_{\mathrm{T}}}$ charged particles and strange hadrons has been exploited.
In this poster, the recent measurement of the near-side jet yield and the out-of-jet yield of $\mathrm{K^0_S}$ and $\Xi$ is shown as a function of the multiplicity of charged particles produced in pp collisions at $\sqrt{s}=13$ TeV. The ratio between the $\Xi$ and the $\mathrm{K^0_S}$ yields is also shown, to highlight the effect of the different strangeness content of the two hadrons.

The results suggest that soft (out of jet) processes are the dominant contribution to strange particle production.

Speaker: Chiara De Martin (Universita e INFN Trieste (IT))

LHCP2021_poster.pdf

Poster video explanation

Zoom meeting room

326 Studies on readout channel thresholds of resistive MicroMegas for ATLAS Muon Spectrometer

ATLAS New Small Wheels upgrade project plans to replace the inner parts of the end-caps of ATLAS Muon Spectrometer with new mechanical structures equipped by a combination of small Thin Gap Chambers (sTGC) and resistive MicroMegas (MM) detectors. During the integration of detectors, the sTGC and MM are separately tested before to be assembled. On MM detectors, tests on the noise are performed together with measurements of tracking efficiency, exploiting the cosmic rays as incoming particles.
The MM readout channels are floating copper strips with different lengths, from 284.0 mm to 1990.0 mm (capacitively coupled with carbon strips at few hundreds V). Due to the wide strip length range, the strip capacitance affects the noise with different magnitude, leading a larger spread in the baseline along a tracking plane, respect to a configuration with same size strips. It also impacts the thresholds that are proportional to baseline rms, with a settable factor. Especially if the variations in thresholds is large among close strips on a tracking layer, it compromises the time measurements for the μTPC procedure.
To uniform the thresholds on the plane, a single-channel level correction can be applied, by an implemented trimmer in the electronic boards (based on VMM ASIC).
Therefore, studies on the baseline and threshold were performed as function of the strip length.
After them, studies on the efficiency and cluster parameters were carried on as function of the thresholds. Their results will be presented.

Speaker: Maria Teresa Camerlingo (Universita e INFN Roma Tre (IT))

LHCP_MTCamerlingo_v07062021.pdf

Zoom link

327 Study of energy deposition patterns in hadron calorimeter for prompt and displaced jets using convolutional neural network

Sophisticated machine learning techniques have promising potential in search for physics beyond Standard Model (BSM) in Large Hadron Collider (LHC). Convolutional neural networks (CNN) can provide powerful tools for differentiating between patterns of calorimeter energy deposits by prompt particles of Standard Model and long-lived particles predicted in various models beyond the Standard Model. We demonstrate the usefulness of CNN by using a couple of physics examples from well motivated BSM scenarios predicting long-lived particles giving rise to displaced jets. Our work suggests that modern machine-learning techniques have the potential to discriminate between energy deposition patterns of prompt and long-lived particles, and thus, they can be useful tools in such searches.

Speaker: Ms Rhitaja Sengupta (Indian Institute of Science, Bengaluru)

lhcp21_rhitaja_poster.pdf

LHCP21_Video

Zoom meeting room

328 Study of the jet transport coefficient at the Large Hadron Collider energies using Color String Percolation Model

Jets are collimated emission of multitude of hadrons which originate from the hard partonic scatterings. They play an important role as hard probes of Quark-gluon plasma (QGP). These hard jets lose their energy through medium-induced gluon radiation and collisonal energy loss. This suppression of final state hadrons at high $p_{\rm T}$ is referred to as jet quenching. Jet quenching is an important signature of QGP and can be characterized by the jet transport parameter ($\hat{q}$), which encodes the parton energy loss in the medium. In this work, we have estimated $\hat{q}$ for $pp$ and AA collisions using the Color String Percolation Model (CSPM). CSPM is a widely used QCD-inspired model which assumes that color strings are stretched between projectile and the target. These color strings can decay into new strings via quark-antiquark pair production and subsequently hadronize to produce observed final state hadrons.

We have studied the jet transport parameter ($\hat{q}$) as a function initial percolation temperature for $pp$ and Pb-Pb collisions at LHC energies. We observe that $\hat{q}$ increases linearly with the increase in initial percolation temperature regardless of the collision system or collision energy. When studied as a function of charged particle multiplicity scaled with the nuclear overlap area, at low multiplicities, $\hat{q}$ shows a sharp increase and this dependency becomes weak at higher multiplicities. This suggests that at lower multiplicities, the system is not dense enough to quench the partonic jets, whereas with increase of multiplicity the jet quenching becomes higher. We have also studied $\hat{q}$ as a function of initial energy density and we found that in the low energy density regime, the system behaves almost like a massless hot pion gas. At higher energy densities, the system deviates from that of the ideal QGP. Finally we have also studied the dimensionless scaled jet transport parameter ($\hat{q}/T^{3}$) which can give us information about the hot and dense partonic medium. We have compared our results obtained from CSPM which has a similar behaviour with that obtained from JET collaboration.

Speaker: Dushmanta Sahu (Indian Institute of Technology Indore (IN))

LHCp-Dushmanta.pdf

Study of the jet transport coefficient at the Large Hadron Collider energies using Color String Percolation Model

329 Tagging the initial state gluon in the Z+jet process

Angularity definition

Angularities are a class of observables of interest for jet phenomenology at the LHC. They are defined by
\begin{equation}
\lambda_\alpha^\kappa=\sum_{i\in\text{jet}}\left(\frac{p_{T, i}}{\sum_{j\in\text{jet}}p_{T, j}}\right)^\kappa \left(\frac{\Delta_i}{R_0}\right)^\alpha
\end{equation}
where $R_0$ is the jet radius and
\begin{equation}
\Delta_i=\sqrt{(y_i-y_\text{jet})^2+(\phi_i-\phi_\text{jet})^2}
\end{equation}
is the Euclidean azimuth-rapidity distance of particle $i$ from the jet axis.
The most standard example of jet angularity is the jet mass corresponding to $\kappa=1$, $\alpha=2$.

A pheno study of jet angularities

In [1] we present a phenomenological study of angularities on the highest transverse-momentum jet in LHC events that feature the associate production of a Z boson and one or more jets. In particular, we study angularity distributions that are measured on jets with and without the Soft Drop grooming procedure. We begin exploring state-of-the-art MC parton shower simulations and we qualitatively assess the impact of NLO matching and merging procedures, then we move to analytic resummation of large logarithms at NLL accuracy. Matching to NLO results is performed in order to achieve NLL' accuracy.

Its application as a jet-flavour tagger

In [2] we use previous results to build a tagger able to determine the flavour of the leading jet in the Z+jet process with some level of confidence. The quark/gluon tagging procedure is achieved through a cut on a jet angularity and it is theoretically well-defined since it exhibits infrared and collinear safety. Now, tagging the flavour of the jet as quark-initiated, we show that it is possible to enhance significantly the initial-state gluon contributions. Exploiting both resummation and MC simulations, we perform a study of their efficiencies and their dependence on non-perturbative effects, for different angularities and different levels of grooming. The first application we want to investigate for our results is to assess in more detail the impact of these types of observable in fits of parton distribution functions.

References:

[1] Jet Angularities in Z+jet production at the LHC - S. Caletti, O. Fedkevych, S. Marzani, D. Reichelt, S. Schumann, G. Soyez, V. Theeuwes; in preparation.
[2] Tagging the initial-state gluon - S. Caletti, O. Fedkevych, S. Marzani, D. Reichelt; in preparation.

Speaker: Mr Simone Caletti (INFN - National Institute for Nuclear Physics)

LHCP21_slide.pdf

LHCP21_video.mp4

Zoom meeting room

330 Testing of the MicroMegas detector trigger electronics for the New Small Wheel Phase I upgrade of ATLAS detector

In conjunction with the High Luminosity upgrade of the LHC, the ATLAS detector is also undergoing an upgrade to handle the significantly higher data rates. The muon end-cap system upgrade in ATLAS, lies with the replacement of Small Wheel. The New Small Wheel is expected to combine high tracking precision with upgraded information for the Level-1 trigger. To accomplish this, sTGC (small Thin Gap Chamber) and MicroMegas (MicroMesh Gas chamber) detector technologies are being deployed.
The MicroMegas detector technology is equipped with three types of electronics boards to produce trigger signals and track muons. These boards are the MMFE8 (MicroMegas Front End with 8 VMM chips), the L1DDC (Level 1 Data Driver Card) and the ADDC (ART Data Driver Card). The ART (Address in Real Time) signals produced by the MMFE8s are propagated through the ADDC and sent to the MicroMegas Trigger Processor for the decision of the Level 1 Accept trigger signal.
In order to test the functionality and efficiency of the trigger electronics, various tests are being conducted at building 899 (BB5). During the "MicroMegas ART connectivity test", internal test pulses are sent through the trigger electronics to simulate ART hits from the Front Ends to the Trigger Processor. This test is performed to validate every New Small Wheel sector and is essential to identify ADDC boards or fibers that must be replaced, tested and then repaired. Issues on MMFE8s and L1DDCs can be identified as well. Finally, the trigger processor's decision logic is being tested with cosmics data. Using the cosmics data, data acquisition, firmware and trigger logic are being improved. In this poster, the various tests and results from cosmics data will be presented.

Speaker: Stamatios Tzanos (National Technical Univ. of Athens (GR))

LHCP_Poster_Tzanos_MM_Triggering.pdf

Zoom meeting

331 The ATLAS Forward Proton Time-of-Flight detector: Projected performance for LHC Run3

We describe the performance of the ATLAS Forward Proton Time-of-Flight detector (ToF) in Run2 and the upgrades made to the ToF for operation in Run3. We describe picosecond laser laboratory test results, previous test beam results, and the expected operational parameters and performance of the new ToF in Run3.

Speaker: Tomas Komarek (Palacky University (CZ))

Komarek_AFP-ToF_Fixed.pdf

Zoom meeting room

332 The ATLAS Level-1 Topological Processor: experience and upgrade plans

During Run-2 the Large Hadron Collider (LHC) has provided, at the World's energy frontier, proton-proton collisions to the ATLAS experiment with high instantaneous luminosity of up to 2.1x10$^{34}$ cm$^{-2}$s$^{-1}$, placing stringent operational and physical requirements on the ATLAS trigger system in order to reduce the 40 MHz collision rate to a manageable event storage rate of 1 kHz, while not rejecting interesting collisions.
The Level-1 trigger is the first rate-reducing step in the ATLAS trigger system with an output rate of up to 100 kHz and decision latency of less than 2.5 microseconds. Since 2017, an important role is played by the Level 1 Topological Processor (L1Topo). This innovative system consists of two blades designed in AdvancedTCA form factor, mounting four individual state-of-the-art processors, and providing high input bandwidth and low latency data processing. Up to 128 topological trigger algorithms can be implemented to select interesting events by applying kinematic and angular requirements on electromagnetic clusters, hadronic jets, muons and total energy reconstructed in the ATLAS apparatus. This resulted in a significantly improved background event rejection rate and improved acceptance of physics signal events, despite the increasing luminosity. The L1Topo system has become more and more important for physics analyses making use of low energy objects, commonly present in the Heavy Flavour or Higgs physics events for example.
In this presentation, an overview of the L1Topo architecture, simulation and performance results during Run-2 is discussed alongside with upgrade plans for the L1Topo system to be installed for the future data taking that will start in 2022.

Speaker: Paula Martinez Suarez (The Barcelona Institute of Science and Technology (BIST) (ES))

PMS_LHCPC_2021_SLIDES.pdf

Zoom meeting room

333 The ATLAS Muon Trigger Design and Performance

Muon triggers are essential for studying a variety of physics processes in the ATLAS experiment, including both standard model measurements and searches for new physics. The ATLAS muon trigger consists of a hardware based system (Level 1), as well as a software based reconstruction (High Level Trigger). The muon triggers have been optimised during Run 2 to provide a high efficiency while keeping the trigger rate low. We will present an overview of how we trigger on muons, recent improvements, the performance of the muon trigger in Run 2 data, and the improvements and the readiness for Run 3.

Speaker: Moe Wakida (Nagoya University (JP))

LHCP2021poster.pdf

Zoom meeting room

334 The ATLAS public website - Evolution to Drupal 8

Four years after the deployment of the ATLAS public website using the Drupal 7 content management system, the ATLAS Education & Outreach group has completed its migration to the new CERN Drupal 8 infrastructure. We present lessons learned from the development, usage and evolution of the original web site, and how the choice of technology helped to shape and reinforce our communication strategy. We then discuss tactics for the migration to Drupal 8, including our choice to use the CERN Override theme. This theme was developed by the CERN web team to support clients like ATLAS to develop web sites in the relatively complex and non-intuitive environment of Drupal. Furthermore, CERN has encouraged usage of this theme to mitigate maintenance and ease future migration. We present the effects this choice has on the design, implementation, and operation of the new site.

Speaker: Mariana Velho (Universidade Nova de Lisboa (PT))

AtlasWeb_LHCPPoster.pdf

Zoom meeting room

335 The characterisation of non-collision background events in the ATLAS detector during LHC Run 2 data-taking.

Understanding events from proton interactions with residual gas in the beam pipe, with collimators or from cosmic rays, is of primary importance to identify potential risk of damage to the accelerator and experiments.
In addition, these events represent one of the main background of non-conventional physics signatures based on tracks not pointing to the interaction point, out-of-time energy deposits, or displaced decay vertices might come from signals released by long-lived heavy particles.
The characteristics of these non-collision backgrounds are illustrated in detail in order to identify, estimate and reject them by using the full ATLAS detector.

Speaker: Zakaria Chadi (Universite Hassan II, Ain Chock (MA))

ATL-COM-DAPR-2021-007-SLIDES.pdf

LHCP_Zakaria-Chadi_7-12-June-2021.pdf

ZOOM poster room

336 The Chirality-Flow Formalism for Standard Model Amplitudes

Scattering amplitudes are often split up into their gauge (su(N)) and kinematic (two copies of complexified su(2)) components. Since the su(N) gauge part is often calculated using flows of colour, it should similarly be possible to describe the su(2) $\oplus$ su(2) kinematics of an amplitude in terms of flows of chirality. In two recent papers (hep-ph:2003.05877 & hep-ph:2011.10075) we showed that this is indeed the case, introducing the chirality-flow formalism for Standard Model calculations. In the chirality-flow method (which simplifies the spinor-helicity method) Feynman diagrams can be directly written down in terms of Lorentz-invariant spinor inner products, allowing the simplest and most direct possible path from Feynman diagram to complex number. In this poster, I will introduce this method and show some examples.

Speaker: Andrew Lifson (Lund University)

ALlhcp.pdf

Poster video explanation

Zoom meeting room

337 The CMS MTD Endcap Timing Layer: Precision Timing with Low Gain Avalanche Detectors

The MIP Timing Detector (MTD) of the Compact Muon Solenoid (CMS) will provide precision timestamps with 40 ps resolution for all charged particles up to a pseudo-rapidity of |η|=3. This upgrade will mitigate the effects of pile-up expected under the High-Luminosity LHC running conditions and bring new and unique capabilities to the CMS detector. The endcap region of the MTD, called the Endcap Timing Layer (ETL), will be instrumented with silicon low gain avalanche detectors (LGADs), covering the high-radiation pseudo-rapidity region 1.6 < |η| < 3.0. The LGADs will be read out with the ETROC readout chip, which is being designed for precision timing measurements. We present recent progress in the characterization of LGAD sensors for the ETL and development of ETROC, including test beam and bench measurements.

Speaker: Christopher Mcmahon (Boston University (US))

The CMS MTD Endcap Timing Layer_ Precision Timing with Low Gain Avalanche Detectors.pdf

Zoom meeting room

338 The contribution of the WLCG Tier-2 site in Prague to the global WLCG operations

Ever since the start of the LHC operations in 2009, the mission of processing, management and storage of data collected by the LHC experiments has been executed by the Worldwide LHC Computing Grid (WLCG). When the building of the infrastructure for LHC computing started (~2001) the distributed or cloud computing was non-existent and the WLCG team had to invent all of the tools from scratch. Gradually, an extensive infrastructure of computing sites spread over 5 continents and interconnected with high capacity internet connectivity was built and continuously upgraded until the current ecosystem of ~ 1 million constantly occupied computer cores, ~ 1 ExaByte of storage and massive global networking with links of 10 – 100 Gb/s throughput. The computing centers involved in WLCG are categorized as Tier 0,1 and 2. Tier-0 is CERN, 14 Tier-1s are large computing centers providing computing power and disk and tape storage. Finally, there are 146 Tier-2 sites mostly universities and scientific institutes, which can store sufficient data and provide adequate computing power for simulation and analysis tasks. Tier-2s represent a very crucial part of the WLCG ecosystem delivering about half of the global WLCG resources.

In this contribution we will present an overview of operations of the Tier-2 site in Prague, Czech republic, which provides computing and storage services for experiments ALICE and ATLAS and also some non-LHC experiments. This overview will show the crucial role of Tier-2 sites in the WLCG considering how many are involved. Our computing center is of a distributed character: the main part of resources is installed at the Institute of Physics (IoP) of the Czech Academy of Sciences (CAS); a part of the XRootD storage cluster for ALICE is operating at the Nuclear Physics Institute (NPI) of the CAS. Smaller clusters of the computing servers are located at the Faculty of Mathematics and Physics of the Charles University, and in CESNET, an association of the Czech Research and Educational institutions. We will provide a detailed overview of the Prague Tier-2 site infrastructure and operations with a special focus on the services provided for the ALICE experiment.

Speaker: Dr Dagmar Adamova (Nuclear Physics Institue of the Czech Academy of Sciences (CZ))

ADAMOVA.LHCp.2021.POSTER.2.pdf

AUDIO.POSTER..WMA

ZOOM LINK FOR POSTER SESSION

339 The Detector Control System of the New Small Wheel for the ATLAS experiment

A series of upgrades are planned for the LHC accelerator to increase it's instantaneous luminosity to 7.5×10$^{34}$ cm$^{-2}$s$^{-1}$. The luminosity increase drastically impacts the ATLAS trigger and readout data rates. The present ATLAS Small Wheel Muon detector will be replaced with a New Small Wheel (NSW) detector which is expected to be installed in the ATLAS underground cavern by the end of the Long Shutdown 2 of the LHC. Due to its complexity and long-term operation, the NSW requires the development of a sophisticated Detector Control System (DCS). The use of such a system is necessary to allow the detector to function consistently and safely as well as to function as a seamless interface to all sub-detectors and the technical infrastructure of the experiment. The central system handles the transition between the probe’s possible operating states while ensuring continuous monitoring and archiving of the system’s operating parameters. Any abnormality in any subsystem of the detector triggers a signal or alert (alarm), which alerts the user and either adapts to automatic processes or allows manual actions to reset the system to function properly.

Speaker: Christos Paraskevopoulos (National Technical Univ. of Athens (GR))

The NSW Detector Control System of the ATLAS experiment LHCP2021, C.Paraskevopoulos.pdf

Zoom meeting room

340 The International Particle Physics Outreach Group - Reaching Across the Globe with Science

The International Particle Physics Outreach Group (IPPOG) is a network of scientists, science educators and communication specialists working across the globe in informal science education and outreach for particle physics. The primary methodology adopted by IPPOG requires the direct involvement of scientists active in current research with education and communication specialists, in order to effectively develop and share best practices in outreach. IPPOG member activities include the International Particle Physics Masterclass programme, International Day of Women and Girls in Science, Worldwide Data Day, International Muon Week and International Cosmic Day organisation, and participation in activities ranging from public talks, festivals, exhibitions, teacher training, student competitions, and open days at local institutions. These independent activities, often carried out in a variety of languages to public with a variety of backgrounds, all serve to gain the public trust and to improve worldwide understanding and support of science. We present our vision of IPPOG as a strategic pillar of particle physics, fundamental research and evidence-based decision-making around the world.

Speaker: Pedro Abreu (LIP Laboratorio de Instrumentacao e Fisica Experimental de Part)

IPPOG_ReachingAcrossGlobeWithScience_Poster_4pages.pdf

IPPOG_ReachingAcrossGlobeWithScience_Poster_A1.pdf

Link to zoom session

341 The LHCb Muon Detector at Upgrade II

The LHCb experiment is a b-physics dedicated experiment at the LHC collider. It has a wide physics program, covering different fields of interest: among others, precise measurements of the CKM matrix elements and the search for lepton flavour violation and beyond Standard Model physics.
The LHCb detector has successfully performed during the Run 1 and Run 2 of the LHC, leading to important contributions in the field of flavour physics as well as physics in the forward region. Now, it is being upgraded in a first step - Upgrade I - to run at a luminosity of 2×1033cm−2s−1. An Upgrade II phase has been proposed, aiming at a full exploitation of the flavour physics potential of the High Luminosity LHC operational period. LHCb Upgrade II will run at instantaneous luminosities of up to 2×1034cm−2s−1 and accumulate a data sample corresponding to a minimum of 300 fb−1.
New design options for the Muon Detector at Upgrade II are under study, in order to deal with the increase in luminosity and readout rate, while preserving the stable operation of the detector and its highly efficient  detection capability. Due to the high variability of the expected particle rates, ranging from several kHz/cm2 in the external regions up to several MHz/cm2 in the inner ones, different sub-detector technologies that could replace or simply complement the old ones are under investigation, with the aim to choose the best option in terms of granularity, radiation hardness and effective spark quenching up to integrated charges of O(C/cm2). An overview of the state of the art of the Muon Detector design for the LHCb Upgrade II will be here presented.

Speaker: Francesco Debernardis (Universita e INFN, Bari (IT))

Francesco_Debernardis_LHCP_10-06_11-06_POSTER.pdf

Zoom meeting room

342 The non-resonant and resonant Higgs pair production at the HL-LHC

A direct measurement of the Higgs self coupling is very crucial to understand the nature of electroweak symmetry breaking. This requires an observation of production of Higgs boson pair, which suffers from very low event rate even at the current LHC run. In our work, we study the prospects of observing the non-resonant Higgs pair production at the high luminosity run of the 14 TeV LHC (HL-LHC). Here, we choose multiple final states based on the event rate and cleanliness, namely, $b\bar{b}\gamma \gamma$, $b\bar{b} \tau^+ \tau^-$, $b\bar{b} WW^*$, $WW^*\gamma \gamma$ and $4W$ channels and do a collider study by employing a cut-based as well as multivariate analyses using the Boosted Decision Tree (BDT) algorithm. Also, we consider various physics beyond the standard model (BSM) scenarios, for example resonant Higgs pair production, to quantify the effects of contamination when one tries to measure the SM di-Higgs signals. In a later study, we search specifically for the heavy resonant scalars ($H/A$) via their decay into two SM Higgs boson at the HL-LHC. After performing multivariate analysis using BDT algorithm in various final states, we set upper limits on the production cross-section of heavy scalar times its branching ratio into final state products for different values of heavy scalar masses. Finally, we translate these limits and put strong constraints on the $m_A-tan\beta$ parameter space (where $m_A$ and $tan\beta$ are respectively the mass of the pseudoscalar and the ratio of the vacuum expectation values of the two Higgs doublets) in the context of Minimal Supersymmetric Standard Model (MSSM).

Speaker: Mr Amit Adhikary (Indian Institute of Science, Bengaluru, India)

LHCP21_poster_AmitAdhikary.pdf

Video presentation.mp4

ZOOM poster room

343 The phase-1 upgrade of the ATLAS level-1 calorimeter trigger

The ATLAS level-1 calorimeter trigger (L1Calo) is a hardware-based system that identifies events containing calorimeter-based physics objects, including electrons, photons, taus, jets, and missing transverse energy. In preparation for Run 3, when the LHC will run at higher energy and instantaneous luminosity, L1Calo is currently implementing a significant programme of planned upgrades. The existing hardware will be replaced by a new system of feature extractor (FEX) modules, which will process finer-granularity information from the calorimeters and execute more sophisticated algorithms to identify physics objects; these upgrades will permit better performance in a challenging high-luminosity and high-pileup environment. This talk will introduce the features of the upgraded L1Calo system and the plans for production, installation, and commissioning. In addition, the expected performance of L1Calo in Run 3 will be discussed.

Speaker: Greg Myers (Indiana University (US))

ATL-COM-DAQ-2021-033.pdf

Zoom meeting room

344 The study on the medium parton distribution from momentum kick model in Heavy-Ion Collisions

The ridge-like structure found in two-particle correlation from the proton-proton collision is one of the hot topics in high-energy heavy-ion physics. Since the medium produced from pp collision is not large enough to generate a high-temperature and high-density medium, called QGP, and therefore this phenomenon can not be suitablely understood through hydrodynamics, unlike in nucleus-nucleus collision.Jet particles lose a considerable amount of energy while they move through the collisions with partons in the medium. The momentum transferred from jets to medium partons are in the direction of jets’ motion, which might produce the collective motion of the medium such as the ridge. In this sense, the momentum kick model has been tested in nucleus-nucleus and pp collisions at various energies. [1]
In this model, the initial parton distribution of the medium is necessary to describe the scattering process kinematically. We have adopted several distribution functions: Maxwell-Boltzmann(MB), Juttner-Synge(JS), and phenomenological parton distribution functions from the soft scattering model (phPDs). However, the MB and JS can not explain a wide range of pseudo-rapidity in the Ridge structure. Therefore we study the phPDs relatively in detail.
The phPDs is parameterized with two variables: the temperature of the medium and a fall-out parameter which determines the decreasing slope at a high-rapidity region. The temperature of the medium critically contibute on the pT distribution while the fall-out parameter on the rapidity distribution. These parameters are determined from the experimental data for pp or AA collisions. [2]
Recently, this model has been used to describe the experimental data for LHC energies, using the parameters fitted to RHIC data, whose energies are 100 times less than LHC energies. Therefore the new study is necessary for the parameter settings for LHC energies.
In this study, we fitted to the simulated data for pp collisions at sqrt{sNN} = 2.76TeV using PYTHIA and new values are quite different from those for low energy data. We compare not only the pT and rapidity distribution but also the lightcone variable distribution. Using these settings, we tried to calculate the two-particle correlations and compare them to the experimental results.

[1] C. Y. Wong, Physical Review C 85, 064909 (2012)
[2] C. Y. Wong, Physical Review C 78, 064905 (2008)
[3] Huh, K. B., Cho, S., Ko, G., & Yoon, J. H. (2018). Two-particle correlation via Bremsstrahlung.
[4] Kim, B., Youn, H., Cho, S. et al. Momentum-Kick Model Application to High-Multiplicity pp Collisions at s√=13 TeV at the LHC. Int J Theor Phys (2021).

Speaker: Soyeon Cho (Inha University (KR))

202106 LHCP The study on the medium parton distribution from momentum kick model in Heavy-Ion Collisions [Poster].pdf

Zoom meeting room

345 The Top-quark electro-weak couplings after LHC run2

Being the heaviest particle of the model, with a mass close to the electroweak scale, the top quark is an interesting candidate for searching for new physics. The electroweak couplings of the top quarks are specially relevant in many extension of the Standard Model. Indeed, as the top-quark was not produced in the previous generation of electron-positron colliders most of its electro-weak couplings can only be constrained with the actual data coming from the Large Hadron Collider. In order to analyse if there is still room for new physics in the electro-weak couplings of the top-quark, we perform a global fit to these couplings. Following the Standard Model Effective Field Theory formalism we have constrained the Wilson coefficients of the dimension six operators that affect the top-quark electro-weak couplings. In this work we consider, for the first time, the QCD corrections at NLO for most of the processes included. Furthermore, we have included recently measured processes, such as $pp\rightarrow tZq$ and $pp\rightarrow t \gamma q$., and the first differential measurements in $pp\rightarrow t\bar{t}Z$ and $pp\rightarrow t\bar{t}\gamma$ production. Taking this into account we are able to improve the bounds significantly with respect to previous results.

Speaker: Marcos Miralles Lopez (IFIC (U.Valencia-CSIC))

LHCP_Marcos_Miralles_poster.pdf

Video Presentation

Zoom meeting room

346 The University of Michigan Semester Research Program at CERN

Since 2013, the University of Michigan has hosted a semester-long research program for undergraduate students at CERN. The students are selected from a diverse mix of small and large universities across the USA and are embedded as CERN Users in active research programs on experiments at the laboratory. The program is modelled on the highly successful NSF-funded Research Experience for Undergraduates (REU) program, which brings 15 students each year to participate in the CERN Summer Student Program, but serves to address the very large demand for additional opportunities during the academic year. CERN mentors are selected due to their leadership skills on the experiments, as well as their ability to educate and inspire the students. Projects cover a wide range of activities from detector R&D to software development, trigger design, physics analysis and theoretical methodology, and touch nearly all aspects of the research program at CERN.

Each semester, around six students, selected from diverse backgrounds, often under-represented in our field, spend three months working at the laboratory. They live in apartment facilities in neighbouring St. Genis Pouilly, and enjoy periodic excursions to cultural centres located around Europe. Funding, which covers travel, per diem and a stipend, has come from a variety of sources, including the Richard Lounsbery Foundation, the University of Michigan Department of Physics, and most recently from the United States Mission to the International Organizations in Geneva. We present the growing success of the program, its strategic interest to the USA, and describe our current efforts to expand and improve its diverse reach to all students across the country.

Speaker: Steven Goldfarb (University of Melbourne (AU))

SemesterAbroadPoster-20210610.pdf

SemesterAbroadSlides-20210610.pdf

Video presentation

Zoom meeting room

347 Transverse spherocity dependence of azimuthal anisotropy in heavy-ion collisions at the LHC using a multi-phase transport model

One of the event shape observables, the transverse spherocity ($S_{0}$), has been studied successfully in small collision systems such as proton-proton collisions at the LHC as a tool to separate jetty and isotropic events. It has unique capability to distinguish events based on their geometrical shapes. In our work, we report the first implementation of transverse spherocity in heavy-ion collisions using a multi-phase transport model (AMPT). We have performed an extensive study of azimuthal anisotropy of charged particles produced in heavy-ion collisions as a function of transverse spherocity ($S_{0}$). We have followed the two-particle correlation (2PC) method to estimate the elliptic flow ($v_2$) in different centrality classes in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV for high-$S_0$, $S_{0}$-integrated and low-$S_0$ events. We have compared the results obtained from AMPT and PYTHIA8 (Angantyr). It is found that two-particle elliptic flow ($v_{2,2}$) is almost zero in the latter one and it is almost free from residual non-flow effects. Also, transverse spherocity does not introduce any bias to the system as far as the elliptic flow is concerned, which is clear from the comparison between the two models. We found that transverse spherocity successfully differentiates heavy-ion collisions’ event topology based on their geometrical shapes i.e. high and low values of spherocity ($S_0$). The high-$S_0$ events are found to have nearly zero elliptic flow while the low-$S_0$ events contribute significantly to elliptic flow of spherocity-integrated events.

Speaker: Mr Neelkamal Mallick (Indian Institute of Technology Indore)

Poster-Sphero-HI-Neelkamal.pdf

video-description-Neelkamal.mp4

Zoom Meeting Link

348 Triggering in ATLAS in Run 2 and Run 3

The ATLAS experiment at the LHC can record about 1 kHz of physics collisions, out of an LHC design bunch crossing rate of 40 MHz. To achieve a high selection efficiency for rare physics events while reducing the significant background rate, a two-level trigger system is used.
The event selection is based on physics signatures, such as the presence of energetic leptons, photons, jets or missing energy. In addition, the trigger system can exploit algorithms using topological information and multivariate methods to carry out the filtering for the many physics analyses pursued by the ATLAS collaboration. In Run 2, around 1500 individual selection paths, the trigger chains, were used for data taking, each with specified rate and bandwidth assignments.
We will give an overview of the Run-2 trigger menu and its performance, allowing the audience to get a taste of the broad physics program that the trigger is supporting. We present the tools that allow us to predict and optimize the trigger rates and CPU consumption for the anticipated LHC luminosities and outline the system to monitor deviations from the individual trigger target rates, and to quickly react to the changing LHC conditions and data taking scenarios.
As an outlook to the upcoming ATLAS data-taking period in Run 3 from 2022 onwards, we present the design principles and ongoing implementation of the new trigger software within the multithreaded framework AthenaMT together with some outlook to the expected performance improvements.

Speaker: Takuya Nobe (University of Tokyo (JP))

LHCP2021.pdf

Zoom meeting room

349 Triggering long-lived particles in HL-LHC and the challenges in the first stage of the trigger system

Triggering long-lived particles (LLPs) at the first stage of the trigger system is very crucial in LLP searches to ensure that we do not miss them at the very beginning. The future High Luminosity runs of the Large Hadron Collider will have an increased number of pile-up events per bunch crossing. There will be major upgrades in hardware, firmware and software sides, like tracking at level-1 (L1). The L1 trigger menu will also be modified to cope with pile-up and maintain the sensitivity to physics processes. In our study we found that the usual level-1 triggers, mostly meant for triggering prompt particles, will not be very efficient for LLP searches in the 140 pile-up environment of HL-LHC, thus pointing to the need to include dedicated L1 triggers in the menu for LLPs. We consider the decay of the LLP into jets and develop dedicated jet triggers using the track information at L1 to select LLP events. We show in our work that these triggers give promising results in identifying LLP events with moderate trigger rates.

Speaker: Prabhat Solanki (Indian Institute of Science, Bengaluru, India)

PSOLANKI_LHCP2021.pdf

ZOOM poster room

350 Upgrade of ATLAS Hadronic Tile Calorimeter for the High Luminosity LHC

The Tile Calorimeter (TileCal) is a sampling hadronic calorimeter covering the central region of the ATLAS experiment, with steel as absorber and plastic scintillators as active medium. The High-Luminosity phase of LHC, delivering five times the LHC nominal instantaneous luminosity, is expected to begin in 2028. TileCal will require new electronics to meet the requirements of a 1 MHz trigger, higher ambient radiation, and to ensure better performance under high pile-up conditions. Both the on- and off-detector TileCal electronics will be replaced during the shutdown of 2025-2027. PMT signals from every TileCal cell will be digitized and sent directly to the back-end electronics, where the signals are reconstructed, stored, and sent to the first level of trigger at a rate of 40 MHz. This will provide better precision of the calorimeter signals used by the trigger system and will allow the development of more complex trigger algorithms. The modular front-end electronics feature radiation-tolerant commercial off-the-shelf components and redundant design to minimise single points of failure. The timing, control and communication interface with the off-detector electronics is implemented with modern Field Programmable Gate Arrays (FPGAs) and high speed fibre optic links running up to 9.6 Gb/s. The TileCal upgrade program has included extensive R&D and test beam studies. A Demonstrator module with reverse compatibility with the existing system was inserted in ATLAS in August 2019 for testing in actual detector conditions. The ongoing developments for on- and off-detector systems, together with expected performance characteristics and results of test-beam campaigns with the electronics prototypes will be discussed.

Speaker: Ryan Peter Mckenzie (University of the Witwatersrand (ZA))

Upgrade of ATLAS Hadronic Tile Calorimeter for The High Luminosity LHC LHCP2021 Slides.pdf

Upgrade of ATLAS Hadronic Tile Calorimeter for the High Luminosity LHC Poster.pdf

Zoom meeting room

351 Upgrades of the ATLAS muon spectrometer with new small-diameter drift tube chambers

After the luminosity upgrade of the Large Hadron Collider (HL-LHC), the rate capability of the muon drift tube detectors of the ATLAS experiment will be exceeded due to the higher particle background rates. In the regions between the inner barrel and endcap of the muon spectrometer the trigger selectivity is limited. Therefore 8 new small diameter (15 mm) Muon Drift Tube chambers (so-called sMDT BIS7A) are installed in the transition regions between the inner barrel and endcap of the muon spectrometer which provide a significant high background rate capability and free space for the installation of new RPC muon trigger chambers as required for operation at HL-LHC. This is a pilot project for the whole replacement of the MDT chambers in the small azimuthal sectors of the barrel inner layer (so-called BIS1-6) by new sMDT-RPC detectors in the long shutdown 3 (LS3). An overview of the validation and installation of the new sMDT BIS7A chambers, their cavern commissioning status and their performance in the ATLAS combined runs during Milestone weeks, will be presented.

Speaker: Ali El Moussaouy (Universite Hassan II, Ain Chock (MA))

Upgrades_of_the_ATLAS_muon_spectrometer_with_new_small-diameter_drift_tube_chambers.pdf

Zoom meeting room

352 Wilson is not anomalous: on gauge anomalies in SMEFT

The use of Effective Field Theories (EFTs) in the search of NP is becoming more and more important given the lack of clear experimental signs of BSM physics. In particular, the Standard Model EFT (SMEFT) has become one of the most popular choices. Hence, the interest in revisiting EFTs is widespread in the community. The importance of chiral anomalies, either in gauge or global symmetries, can not be overstated because of their phenomenological and formal importance. A natural question then arise: can higher-dimensional operators in an EFT generate gauge anomalies if the renormalizable part of the EFT is anomaly-free? I will discuss whether dimension-6 operators in SMEFT can induce gauge anomalies. We find a negative answer, contrarily to what was claimed by Cata et al in a recent paper (2011.09976) and therefore I'll discuss why the triangle-diagram computations performed in the aforementioned paper lead to apparent anomalies. I will provide arguments based on conserved currents and a more innovative derivation based on the smart construction of an EFT. Poster based on 2012.07740.

Speaker: Alejo Rossia (Deutsches Elektronen-Synchrotron DESY)

Wilson_is_not_anomalous.pdf

ZOOM poster room

Friday 11 June

Poster Session

Plenary VII: QCD Physics

Conveners: Laure Marie Massacrier (Université Paris-Saclay (FR)), Mika Anton Vesterinen (University of Warwick (GB))

353 Precision QCD theory

Speaker: Claude Duhr (CERN)

lhcp21_duhr.pdf

Recording

354 Results on vector boson (+jet) production

Speaker: Daniel Charles Craik (Massachusetts Inst. of Technology (US))

20210611_dcraik_lhcp_v5.pdf

Recording

355 Jet properties and substructure (theory)

Speaker: Mrinal Dasgupta (University of Manchester (GB))

md-lhcp-2021.pdf

Recording

356 Jet properties and substructure (exp)

Speaker: Leticia Cunqueiro Mendez (Oak Ridge National Laboratory - (US))

Cunqueiro_LHCP21_finald.pdf

Recording

357 Results on soft QCD at LHC and Tevatron

Speaker: Leszek Adamczyk (AGH University of Science and Technology (PL))

Adamczyk.pdf

Recording

14:00 Coffee break

Plenary VIII: Heavy Ions

Conveners: Eero Aleksi Kurkela (University of Stavanger (NO)), Roberta Arnaldi (Universita e INFN Torino (IT))

358 Heavy ion collisions - theory

Speaker: Jasmine Therese Brewer (CERN)

JasmineBrewer-LHCP2021.pdf

Recording

359 Hard probes of QGP

Speaker: Laura Brittany Havener (Yale University (US))

LHCP_HardProbesQGP_Havener_v7.pdf

Recording

360 Understanding QGP with heavy flavor and quarkonia

Speaker: Sebastian Tapia Araya (Univ. Illinois at Urbana Champaign (US))

LHCP_HF_stapia_V5.pdf

Recording

361 Soft particle production from QGP

Speaker: Alice Ohlson (Lund University (SE))

aohlson_lhcp21.pdf

Recording

16:15 Coffee break

Plenary IX: Upgrades

Conveners: Marco Van Leeuwen (Nikhef National institute for subatomic physics (NL)), Patricia McBride (Fermi National Accelerator Laboratory (FNAL))

362 Upgrades for ALICE

Speaker: Christian Lippmann (GSI - Helmholtzzentrum fur Schwerionenforschung GmbH (DE))

ALICE_TPC_track_movie_fast_11TF_20210309.mp4

Lippmann_ALICE_Upgrades_v7.pdf

Recording

363 Upgrades for ATLAS

Speaker: Richard Teuscher (University of Toronto (CA))

ATLAS-Upgrades-Teuscher.pdf

Recording

364 Upgrades for CMS

Speaker: Santiago Folgueras (Universidad de Oviedo (ES))

LHCP_CMSUpgrades_Folgueras.pdf

Recording

365 Upgrades for LHCb

Speaker: Tomasz Szumlak (AGH University of Science and Technology (PL))

lhcb_upgrades_LHCP.2021.T.Szumlak.pdf

Recording

366 Physics at the HL-LHC and beyond

Speaker: Sergo Jindariani (Fermi National Accelerator Lab. (US))

LHCP2021_PhysicsAtFutureColliders.pdf

Recording

Saturday 12 June

Closing Plenary

Conveners: Cheng-Wei Chiang (National Taiwan University), Dave Charlton (University of Birmingham (GB)), Kai-Feng Chen (National Taiwan University (TW))

367 Closing remarks from the LHCP2021 International Advisory Committee

Speaker: Bruno Mansoulie (Université Paris-Saclay (FR))

LHCP2021_IAC-report_closing.pdf

Recording

368 Poster awards ceremony

Committee: Johannes Albrecht, Maria Cepeda Hermida, Tristan du Pree, Elisabetta Gallo (chair), Stefania Gori, Heather Gray, Yvonne Pachmeyer, Marek Schoenherr, José Francisco Zurita

Speaker: Elisabetta Gallo (DESY)

LHCP_posters_finalchoice.pdf

Recording

369 Report from the LHC Early Career Scientists Fora

Speaker: Igor Kostiuk (Nikhef National institute for subatomic physics (NL))

IK_LHCP_fora_2021-v3.pdf

Recording

370 Keynote talk: Dark matter

Speaker: Laura Baudis (University of Zurich)

baudis_lhcp2021.pdf

Recording

371 LHCP2021 experimental highlights

Speaker: Shahram Rahatlou (Sapienza Universita e INFN, Roma I (IT))

rahatlou-lhcp2021.pdf

Recording

372 Theory vision

Speaker: Gian Giudice (CERN)

LHCP21Giudice2.pdf

Recording

373 Closing remarks

Speakers: Dave Charlton (University of Birmingham (GB)), Tulika Bose (University of Wisconsin Madison (US))

LHCP2021-ClosingRemarks.pdf

Recording