25–30 May 2020
Europe/Paris timezone
There is a live webcast for this event.

Contribution List

263 out of 263 displayed
Export to PDF
  1. Giovanni Marchiori (LPNHE Paris), Roberto Salerno (Centre National de la Recherche Scientifique (FR))
    25/05/2020, 12:30
  2. Jose Miguel Jimenez (CERN)
    25/05/2020, 12:40
  3. Andrea Dainese (INFN - Padova (IT))
    25/05/2020, 13:05
  4. Klaus Monig (Deutsches Elektronen-Synchrotron (DE))
    25/05/2020, 13:30
  5. Patricia Mcbride (Fermi National Accelerator Lab. (US))
    25/05/2020, 13:55
  6. Matthew John Charles (Sorbonne Université / LPNHE)
    25/05/2020, 14:20
  7. Alexis Vallier (CERN)
    25/05/2020, 15:00
  8. Krzysztof Kutak (Instytut Fizyki Jadrowej Polskiej Akademii Nauk)
    25/05/2020, 15:00
    Talk
  9. Aishik Ghosh (Université Paris-Saclay (FR))
    25/05/2020, 15:00
    Talk
  10. Dr Tim Stefaniak (DESY)
    25/05/2020, 15:00
  11. Giuseppe Bevilacqua (Unideb (Hungary))
    25/05/2020, 15:00
  12. Roberto Preghenella (INFN, Bologna (IT))
    25/05/2020, 15:00
  13. Mattia Faggin (Universita e INFN, Padova (IT))
    25/05/2020, 15:00
    Performance
    Talk
  14. Carlos Francisco Erice Cid (Universidad de Oviedo (ES))
    25/05/2020, 15:18
  15. Ilya Gorbunov (Joint Institute for Nuclear Research (RU))
    25/05/2020, 15:18
  16. Anja Butter
    25/05/2020, 15:18
    Talk
  17. Petr Jacka (Czech Academy of Sciences (CZ))
    25/05/2020, 15:18
  18. Mariusz Przybycien (AGH University of Science and Technology (PL))
    25/05/2020, 15:18
    Talk
  19. Christopher Betancourt (Universitaet Zuerich (CH))
    25/05/2020, 15:18
  20. Renata Kopecna (Ruprecht Karls Universitaet Heidelberg (DE))
    25/05/2020, 15:18
  21. Mark Hodgkinson (University of Sheffield (GB))
    25/05/2020, 15:36
  22. Menglin Xu (Central China Normal University CCNU (CN))
    25/05/2020, 15:36
  23. Javier Cuevas (Universidad de Oviedo (ES))
    25/05/2020, 15:36
  24. Enrico Bothmann (University of Göttingen)
    25/05/2020, 15:36
    Talk
  25. Alena Harlenderova (GSI - Helmholtzzentrum fur Schwerionenforschung GmbH (DE))
    25/05/2020, 15:36
    Talk
  26. Dr Djamel Eddine Boumediene (Université Clermont Auvergne (FR))
    25/05/2020, 15:36
  27. Salvador Marti I Garcia (IFIC-Valencia (UV/EG-CSIC))
    25/05/2020, 15:36
  28. Barbara Alvarez Gonzalez (Universidad de Oviedo (ES))
    25/05/2020, 15:54
  29. Stefano Carrazza (CERN)
    25/05/2020, 15:54
    Talk
  30. William Shepherd (Sam Houston State University)
    25/05/2020, 15:54
  31. Émilien Chapon (Chinese Academy of Sciences (CN))
    25/05/2020, 15:54
    Talk
  32. Mateusz Zarucki (HEPHY)
    25/05/2020, 15:54
  33. Izaak Neutelings (Universitaet Zuerich (CH))
    25/05/2020, 15:54
  34. Pablo Martinez Ruiz Del Arbol (Universidad de Cantabria and CSIC (ES))
    25/05/2020, 15:54
  35. Piotr Gasik (GSI - Helmholtzzentrum fur Schwerionenforschung GmbH (DE))
    25/05/2020, 16:45
    Talk
  36. Vincenzo Izzo (Universita e sezione INFN di Napoli (IT))
    25/05/2020, 17:10
    Talk
  37. Marcello Mannelli (CERN)
    25/05/2020, 17:35
    Talk
  38. Mark Tobin (Chinese Academy of Sciences (CN))
    25/05/2020, 18:00
    Talk
  39. Fabio Maltoni (Universite Catholique de Louvain (UCL) (BE))
    26/05/2020, 12:30
    Talk
  40. Geoffrey Gilles (Bergische Universitaet Wuppertal (DE))
    26/05/2020, 13:00
    Talk
  41. Efe Yazgan (National Taiwan University (TW))
    26/05/2020, 13:30
    Talk
  42. Elizaveta Shabalina (Georg August Universitaet Goettingen (DE))
    26/05/2020, 14:00
    Talk
  43. Rafael Teixeira De Lima (SLAC National Accelerator Laboratory (US))
    26/05/2020, 14:45
  44. Matteo Concas (INFN e Politecnico di Torino (IT))
    26/05/2020, 14:45
    Talk
  45. Rajdeep Mohan Chatterjee (University of Minnesota (US))
    26/05/2020, 14:45
  46. Shilpi Jain (University of Minnesota (US))
    26/05/2020, 14:45
  47. Aidan Grummer (University of New Mexico (US))
    26/05/2020, 14:45
  48. Marjorie Shapiro (Lawrence Berkeley National Lab. (US))
    26/05/2020, 14:45
  49. Fady Adibsamy Bishara (DESY), Fady Bishara (University of Oxford)
    26/05/2020, 14:45
  50. William Axel Leight (DESY)
    26/05/2020, 15:00
  51. Jacco Andreas De Vries (Universiteit Maastricht (NL))
    26/05/2020, 15:03
  52. Alex Seuthe (Technische Universitaet Dortmund (DE))
    26/05/2020, 15:03
  53. Jon Burr (Deutsches Elektronen-Synchrotron (DE))
    26/05/2020, 15:03
  54. Vladimir Gligorov (Centre National de la Recherche Scientifique (FR))
    26/05/2020, 15:03
    Talk
  55. Giacomo Zecchinelli (Imperial College (GB))
    26/05/2020, 15:03
  56. Sandhya Jain (Centre National de la Recherche Scientifique (FR))
    26/05/2020, 15:03
  57. Andrea Gabrielli (Lawrence Berkeley National Lab. (US))
    26/05/2020, 15:15
  58. Peter Loch (University of Arizona (US))
    26/05/2020, 15:21
  59. Milos Dordevic (Vinca Institute, University of Belgrade)
    26/05/2020, 15:21
  60. Miriam Lucio Martinez (Nikhef National institute for subatomic physics (NL))
    26/05/2020, 15:21
  61. Loukas Gouskos (CERN)
    26/05/2020, 15:21
    Talk
  62. Nicola Neri (Università degli Studi e INFN Milano (IT))
    26/05/2020, 15:21
  63. Varun Sharma (University of Wisconsin Madison (US))
    26/05/2020, 15:21
  64. Mathieu Pellen (University of Cambridge)
    26/05/2020, 15:21
  65. Xuan Chen (Universitaet Zuerich (CH))
    26/05/2020, 15:30
  66. Laura Brittany Havener (Yale University (US))
    26/05/2020, 15:39
    Talk
  67. Fabrizio Grosa (Universita e INFN Torino (IT))
    26/05/2020, 15:39
  68. Douglas Michael Schaefer (University of Chicago (US))
    26/05/2020, 15:39
  69. Admir Greljo (CERN)
    26/05/2020, 15:39
  70. Matthew Lim (Milano-Biccoca)
    26/05/2020, 15:45
  71. Thomas Kurt Gehrmann (Universitaet Zuerich (CH))
    26/05/2020, 16:30
  72. Gregory Soyez (IPhT, CEA Saclay)
    26/05/2020, 17:00
  73. William Barter (Imperial College (GB))
    26/05/2020, 17:30
  74. Valentina Zaccolo (Universita e INFN Trieste (IT))
    26/05/2020, 18:00
  75. Wilke Van Der Schee (MIT)
    27/05/2020, 12:30
    Talk
  76. Yi Chen (Massachusetts Inst. of Technology (US))
    27/05/2020, 13:00
    Talk
  77. Gian Michele Innocenti (CERN)
    27/05/2020, 13:30
    Talk
  78. Livio Bianchi (Universita e INFN Torino (IT))
    27/05/2020, 14:00
    Talk
  79. Sook Hyun Lee (University of Michigan (US))
    27/05/2020, 14:45
  80. Stefano Augusto Pozzorini (Universitaet Zuerich (CH))
    27/05/2020, 14:45
  81. Ben Nachman (Lawrence Berkeley National Lab. (US))
    27/05/2020, 14:45
    Talk
  82. Magdalena Djordjevic (Institute of Physics Belgrade)
    27/05/2020, 14:45
    Talk
  83. Olena Karacheban (Rutgers State Univ. of New Jersey (US))
    27/05/2020, 14:45
  84. Richard Ruiz (Universite Catholique de Louvain)
    27/05/2020, 14:45
  85. Davide Pagani (Deutsches Elektronen-Synchrotron (DE))
    27/05/2020, 14:45
  86. David Dobrigkeit Chinellato (University of Campinas UNICAMP (BR))
    27/05/2020, 15:03
  87. David Shih (Rutgers University)
    27/05/2020, 15:03
    Talk
  88. Michal Szleper, Michal Szleper (National Centre for Nuclear Research (PL))
    27/05/2020, 15:03
  89. Robert Vertesi (Wigner Research Centre for Physics (Wigner RCP) (HU))
    27/05/2020, 15:03
  90. Christopher Young (CERN)
    27/05/2020, 15:03
  91. Alexandre Lebedev (Iowa State University)
    27/05/2020, 15:03
    Talk
  92. Adam Bailey (Univ. of Valencia and CSIC (ES))
    27/05/2020, 15:03
  93. Lukas Alexander Heinrich (CERN)
    27/05/2020, 15:21
    Talk
  94. Alessandro Da Rold (Universita e INFN Trieste (IT))
    27/05/2020, 15:21
  95. Matt LeBlanc (University of Arizona (US))
    27/05/2020, 15:21
  96. Dorothea Vom Bruch (LPNHE Paris, CNRS)
    27/05/2020, 15:21
  97. Joscha Knolle (Deutsches Elektronen-Synchrotron (DE))
    27/05/2020, 15:21
  98. Chun-Lu Huang (Université Paris-Saclay (FR))
    27/05/2020, 15:21
    Talk
  99. Renjie Wang (Johannes Gutenberg-Universität Mainz (DE))
    27/05/2020, 15:21
  100. David Rohr (CERN)
    27/05/2020, 15:39
  101. Sezen Sekmen (Kyungpook National University (KR))
    27/05/2020, 15:39
    Talk
  102. Ruchi Gupta (Deutsches Elektronen-Synchrotron (DE))
    27/05/2020, 15:39
  103. Matteo Negrini (Universita e INFN, Bologna (IT))
    27/05/2020, 15:39
  104. Joao Pires (LIP Lisboa)
    27/05/2020, 15:39
  105. Dr Benjamin Audurier (Centre national de la recherche scientifique)
    27/05/2020, 15:39
    Talk
  106. Ke Li (University of Washington (US))
    27/05/2020, 15:39
  107. Sally Dawson, Sara Lynn Dawson
    27/05/2020, 16:30
    Talk
  108. Luca Fiorini (Univ. of Valencia and CSIC (ES))
    27/05/2020, 17:00
    Talk
  109. Milada Muhlleitner, Milada Muhlleitner (KIT - Karlsruhe Institute of Technology (DE))
    27/05/2020, 17:30
    Talk
  110. Giovanni Petrucciani (CERN)
    27/05/2020, 18:00
    Talk
  111. Alessandro Vicini (Università degli Studi e INFN Milano (IT))
    28/05/2020, 12:30
    Talk
  112. Ludovica Aperio Bella (Deutsches Elektronen-Synchrotron (DE))
    28/05/2020, 13:00
    Talk
  113. Saptaparna Bhattacharya (Northwestern University (US))
    28/05/2020, 13:30
    Talk
  114. Christian Gutschow (UCL (UK))
    28/05/2020, 14:00
    Talk
  115. Guillaume Max Pietrzyk (EPFL - Ecole Polytechnique Federale Lausanne (CH))
    28/05/2020, 14:45
  116. Andrey Pozdnyakov (Rheinisch Westfaelische Tech. Hoch. (DE))
    28/05/2020, 14:45
  117. Michele Selvaggi (CERN)
    28/05/2020, 14:45
  118. Dr Aleksas Mazeliauskas (CERN)
    28/05/2020, 14:45
    Talk
  119. Charlotte Van Hulse (University College Dublin (IE))
    28/05/2020, 14:45
  120. Zhen Liu (U of Maryland)
    28/05/2020, 14:45
  121. Beth Bramley
    28/05/2020, 14:45
    Outreach
    Talk
  122. Stephen Jiggins (Albert Ludwigs Universitaet Freiburg (DE))
    28/05/2020, 15:00
  123. Zhanna Khabanova (Nikhef National institute for subatomic physics (NL))
    28/05/2020, 15:03
    Talk
  124. Prof. Jonathan Butterworth (UCL)
    28/05/2020, 15:03
    Outreach
    Talk
  125. Allison Reinsvold Hall (Fermilab)
    28/05/2020, 15:03
  126. Alberto Caliva (GSI - Helmholtzzentrum fur Schwerionenforschung GmbH (DE))
    28/05/2020, 15:03
  127. Nico Gubernari (technische universität münchen)
    28/05/2020, 15:05
  128. Andrea Wulzer (CERN and EPFL)
    28/05/2020, 15:09
  129. Seraina Glaus (KIT)
    28/05/2020, 15:15
  130. Uta Bilow (Technische Universitaet Dresden (DE))
    28/05/2020, 15:21
    Outreach
    Talk
  131. Michael Murray (The University of Kansas (US))
    28/05/2020, 15:21
    Talk
  132. Masahiko Saito (University of Tokyo (JP))
    28/05/2020, 15:21
  133. Peter John Bussey (University of Glasgow (GB))
    28/05/2020, 15:21
  134. Mirco Dorigo (INFN Trieste)
    28/05/2020, 15:25
  135. Daniel Guerrero (University of Florida (US))
    28/05/2020, 15:30
  136. Daniel Schulte (CERN)
    28/05/2020, 15:33
  137. James Lawrence Nagle (University of Colorado Boulder)
    28/05/2020, 15:39
    Talk
  138. Prof. Hans Peter Beck (Universitaet Bern (CH))
    28/05/2020, 15:39
    Outreach
    Talk
  139. Marcin Kucharczyk (Polish Academy of Sciences (PL))
    28/05/2020, 15:39
  140. Deniz Sunar Cerci (Adiyaman University (TR) - Istanbul University (TR))
    28/05/2020, 15:39
  141. Stefano Manzoni (Nikhef National institute for subatomic physics (NL))
    28/05/2020, 15:50
  142. Alexis Kalogeropoulos (Princeton University)
    28/05/2020, 16:30
  143. Ines Ochoa (Columbia University (US))
    28/05/2020, 17:00
  144. Elina Fuchs (Fermilab & University of Chicago)
    28/05/2020, 17:30
  145. Ken Mimasu (Université Catholique de Louvain)
    28/05/2020, 18:00
  146. Ms Yanchun Ding ( CCNU (CN), LYON-IP2I(FR))
    28/05/2020, 18:45
    Heavy Ions
    Experimental poster

    In pp collisions at LHC energies, the production of heavy quarks proceeds from the hard scattering and then these quarks hadronise in either open heavy-flavor hadrons or quarkonia (e.g. J/$\psi$, $\psi(2S)$, $\Upsilon$). The study of quarkonium production as a function of charged-particle multiplicity links soft and hard processes and allows to study their interplay. While a linear increase of...

    Go to contribution page
  147. Carlos Francisco Erice Cid (Universidad de Oviedo (ES))
    28/05/2020, 18:45
    Upgrade & Future
    Experimental poster

    The electronics of the CMS (Compact Muon Solenoid) DT (Drift Tubes) chambers will need to be replaced for the HL-LHC (High Luminosity Large Hadron Collider) operation due to the increase of occupancy and trigger rates in the detector, which cannot be sustained by present system. A system is being designed that will forward asynchronously the totality of the chambers signals to the control...

    Go to contribution page
  148. David Horak (Czech Technical University (CZ))
    28/05/2020, 18:45
    Heavy Ions
    Experimental poster

    The powerful photon fluxes of relativistic nuclei provide the possibility to study photonuclear and two-photon interactions in ultra-peripheral collisions (UPC), where the nuclei do not overlap and no strong nuclear interactions occur. Within the Vector Meson Dominance Model (VDM), the rho0 contribution dominates the QCD part of the photon structure function. The gamma+A → rho0+A process in...

    Go to contribution page
  149. Sana Ketabchi (University of Toronto (CA))
    28/05/2020, 18:45
    Upgrade & Future
    Experimental poster

    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...

    Go to contribution page
  150. Takuya Nobe (University of Tokyo (JP))
    28/05/2020, 18:45
    Upgrade & Future
    Experimental poster

    The LHC is expected to increase its centre-of-mass energy to 14 TeV and to keep longer time with an instantaneous luminosity of about 2.0×10^34 cm^-2s^-1 for Run-3 scheduled from 2021 to 2024. In order to cope with the high event rate, upgrades of the ATLAS trigger system are required. The level-1 Endcap Muon trigger system identifies muons with high transverse momentum by combining data from...

    Go to contribution page
  151. Meirin Oan Evans (University of Sussex (GB))
    28/05/2020, 18:45
    Outreach
    Experimental poster

    Modern particle physics analysis is carried out using sophisticated programming and coding. How, therefore, can we genuinely introduce students to experimental particle physics analysis without an initial exposure to the coding behind? The answer from ATLAS Open Data is to build tools for interactive data visualisation. Web-based resources such as the “Histogram Analyser”, “ATLAS detector...

    Go to contribution page
  152. Ana Peixoto (LIP Laboratorio de Instrumentacao e Fisica Experimental de Part)
    28/05/2020, 18:45
    Outreach
    Experimental poster

    The ATLAS experiment at the Large Hadron Collider is collecting unprecedented amounts of proton–proton collision data. The ATLAS Collaboration analyses these data, seeking to give answers to questions that have puzzled particle physicists for many decades now. In this process, the Standard Model is being precisely measured and searches for new physics are performed in sophisticated and clever...

    Go to contribution page
  153. Muhammad Alhroob (University of Oklahoma (US))
    28/05/2020, 18:45
    Outreach
    Experimental poster

    The Virtual Visit service run by the ATLAS Collaboration has been provided since 2010. The ATLAS Collaboration has used this popular and effective method to bring the excitement of scientific exploration and discovery into classrooms and other public places around the world. The programme, which uses a combination of video conferencing, webcasts, and video recording to communicate with remote...

    Go to contribution page
  154. Mr Axel Buchot Perraguin (Centre National de la Recherche Scientifique (FR))
    28/05/2020, 18:45
    Upgrade & Future
    Experimental poster

    The existing CMS endcap calorimeters will be replaced with a High Granularity Calorimeter (HGCAL) for operation at the High-Luminosity (HL) LHC. Radiation hardness and excellent physics performance will be achieved by utilising silicon pad sensors and SiPM-on-scintillator tiles with high transverse and longitudinal segmentation. One of the major challenges of the HL-LHC will be the high pileup...

    Go to contribution page
  155. Joscha Knolle (Deutsches Elektronen-Synchrotron (DE))
    28/05/2020, 18:45
    Performance
    Experimental poster

    The luminosity measurement of the CMS experiment is calibrated under special beam conditions with beam separation scans called Van der Meer (VdM) scans. In a VdM scan, the two proton beams are separated transversely and moved in steps across each other. From the rate measurement of a luminosity detector as function of the transverse beam separation, the absolute luminosity scale is inferred...

    Go to contribution page
  156. Yong Du (University of Massachusetts-Amherst)
    28/05/2020, 18:45
    Dark Sector BSM
    Theory poster

    We study discovery prospects for a real triplet extension of the Standard Model scalar sector at the Large Hadron Collider (LHC) and a possible future 100TeV $pp$ collider. We focus on the scenario in which the neutral triplet scalar is stable and contributes to the dark matter relic density. When produced in $pp$ collisions, the charged triplet scalar decays to the neutral component plus a...

    Go to contribution page
  157. Devanshu Kiran Panchal (University of Texas at Austin (US))
    28/05/2020, 18:45
    Upgrade & Future
    Experimental poster

    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...

    Go to contribution page
  158. Ms Pooja Pareek (Variable Energy Cyclotron Centre (IN))
    28/05/2020, 18:45
    QCD physics
    Experimental poster

    We present in this poster the measurement of light neutral mesons, $\pi^{0}$ and $\eta$, in pp collisions at different center-of-mass energies obtained with the ALICE experiment at CERN. In pp collisions, neutral mesons are used to validate the pQCD predictions and also act as a baseline for their measurement in heavy-ion collisions. Neutral mesons have been reconstructed by invariant mass...

    Go to contribution page
  159. Emma Torro Pastor (Univ. of Valencia and CSIC (ES))
    28/05/2020, 18:45
    Dark Sector BSM
    Experimental poster

    MATHUSLA is a proposed detector that will be placed above the CMS experiment to study long-lived particles (LLP) produced by the LHC. It is instrumented with a tracking system to observe LLP decays inside its empty volume, and it is composed of a modular array of detectors covering together (100 × 100) m2 × 25 m high. MATHUSLA, with a large detection area and good granularity tracking system,...

    Go to contribution page
  160. Mr Rajeev Singh (Institute of Nuclear Physics Polish Academy of Sciences)
    28/05/2020, 18:45
    Heavy Ions
    Theory poster

    Measurements made recently by the STAR collaboration show that the Lambda hyperons produced in relativistic heavy-ion collisions are subject to global spin polarization with respect to an axis coincident with the axis of rotation of the produced matter. Recently formulated formalism of relativistic hydrodynamics with spin, which is a generalization of the standard hydrodynamics, is a natural...

    Go to contribution page
  161. Jonas Wurzinger (University of Oxford (GB))
    28/05/2020, 18:45
    Performance
    Experimental poster

    Transverse missing momentum from non-interacting particles is one of the important characteristics for many analyses especially for Beyond Standard Model physics searches. To study these events at the Large Hadron Collider (LHC) with the ATLAS experiment an efficient trigger selection is needed. The ATLAS transverse missing momentum trigger uses calorimeter-based global energy sums together...

    Go to contribution page
  162. Dr Sandeep Bhowmik (National Institute of Chemical Physics and Biophysics (EE))
    28/05/2020, 18:45
    Upgrade & Future
    Experimental poster

    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 as well as searches for new physics beyond the standard model. The Compact Muon Solenoid (CMS) experiment is planning to replace entirely its trigger and data acquisition system to achieve this ambitious physics program. Efficiently...

    Go to contribution page
  163. LINGFENG LI (HKUST)
    28/05/2020, 18:45
    Upgrade & Future
    Theory poster

    Information deformation and loss in jet clustering are one of the major limitations for precisely measuring hadronic events at future $e^-e^+$ colliders. Because of their dominance in data, the measurements of such events are crucial for advancing the precision frontier of Higgs and electroweak physics in the next decades. We show that this difficulty can be well-addressed by synergizing the...

    Go to contribution page
  164. Chiara Pinto (INFN and University of Catania)
    28/05/2020, 18:45
    Heavy Ions
    Experimental poster

    The measurement of (anti)nuclei production in pp, p-A and A-A collisions at the ultrarelativistic energies of LHC is important to understand hadronization. The excellent tracking and particle identification capabilities of ALICE make it the most suited detector at the LHC to study light (anti)nuclei produced in high-energy hadronic collisions. (Anti)nuclei with mass numbers up to 4, such as...

    Go to contribution page
  165. Giovanni Bartolini (CPPM, Aix-Marseille Université, CNRS/IN2P3 (FR))
    28/05/2020, 18:45
    Performance
    Experimental poster

    The identification of jets coming from the hadronization of b-quarks (b-tagging) is instrumental for many physics analyses performed at the Large Hadron Collider. ATLAS has b-tagging capability starting at trigger level, where b-tagging algorithms are fed with tracks that are reconstructed at the High-Level Trigger stage. Physics analyses with b-jets in the final state, but no lepton or...

    Go to contribution page
  166. Konie Al Khoury (Université Paris-Saclay (FR))
    28/05/2020, 18:45
    Higgs physics
    Experimental poster

    The Higgs boson decays to pairs of b-quarks were studied in associated production with a W or Z boson by the ATLAS Collaboration. The decay to b-quarks is of particular importance since it allows a direct measurement of the coupling of the Higgs boson to b-quarks. The highest sensitivity in this channel is obtained when the vector boson produced alongside the Higgs boson decays to leptons. The...

    Go to contribution page
  167. Mr Claudio Andrea Manzari (University of Zurich)
    28/05/2020, 18:45
    Flavour physics
    Theory poster

    Recently, discrepancies of up to 4σ between the different determinations of the CKM element Vus have been observed. Modified neutrino couplings to Standard Model gauge bosons could explain this "Cabibbo-angle anomaly". However, this explanation necessarily affects also the EW fit and the other observables sensitive to LFU violation. Therefore, in order to assess the viability, a global fit of...

    Go to contribution page
  168. Ms SURABHI GUPTA (Aligarh Muslim University)
    28/05/2020, 18:45
    Higgs physics
    Theory poster

    The discovery of a 125 GeV Higgs-boson at the Large Hadron Collider poses a significant challenge for the minimal supersymmetric standard model (MSSM). We present our phenomenological research on various Higgs allied processes in the light of the pre-existing data from several other experiments including the data on electroweak precision observables, B-physics and the data from dark matter...

    Go to contribution page
  169. Manuel Guth (Albert Ludwigs Universitaet Freiburg (DE))
    28/05/2020, 18:45
    Performance
    Experimental poster

    The identification of heavy flavour jets (tagging) plays an important role in many
    physics analyses at the ATLAS experiment. It is an essential tool for precision measurements as well as for searches for new physics phenomena. Significant progress has been made in the last few years to ensure the robust training of deep neural networks, requiring large training datasets.
    The ATLAS deep...

    Go to contribution page
  170. Elena Michelle Villhauer (The University of Edinburgh (GB))
    28/05/2020, 18:45
    Upgrade & Future
    Experimental poster

    The Run 2 ATLAS trigger system is comprised of two levels: a hardware level (L1) and a software higher level trigger (HLT). Between late 2018 and early 2021, the ATLAS trigger system is undergoing upgrades. Two major sets of upgrades to the ATLAS level 1 trigger system will be the increase in read-out granularity in the LAr detectors ("supercells") and the addition of new Feature EXtractors...

    Go to contribution page
  171. Mahmoud Gadallah (Eotvos Lorand University (HU))
    28/05/2020, 18:45
    Performance
    Experimental poster

    Precise luminosity calibration at bunched-beam hadron colliders like the Large Hadron Collider (LHC) is critical to determine fundamental parameters of the standard model and to constrain or to discover beyond-the-standard-model phenomena. The luminosity determination at the LHC interaction point 5 with the Compact Muon Solenoid (CMS) detector, using proton-proton, proton-nucleus, or...

    Go to contribution page
  172. Emil Gorm Nielsen (University of Copenhagen (DK))
    28/05/2020, 18:45
    Heavy Ions
    Experimental poster

    Emil Gorm Nielsen (on behalf of the ALICE Collaboration)
    Niels Bohr Institute, University of Copenhagen, Denmark

    One of the main goals of ultra-relativistic nuclear collisions is to create a
    new state of matter called quark-gluon plasma (QGP) and study its properties. One of the experimental observables is the anisotropic flow vn, defined
    as correlation of azimuthal angle of each...

    Go to contribution page
  173. Dr Bin Yan (Los Alamos National Laboratory)
    28/05/2020, 18:45
    Electroweak physics
    Theory poster

    We propose to utilize the polarization information of the $Z$ bosons in $ZZ$ production, via the gluon-gluon fusion process $gg\to ZZ$, to probe the $Zt\bar{t}$ gauge coupling. The contribution of longitudinally polarized $Z$ bosons is sensitive to the axial-vector component ($a_t$) of the $Zt\bar{t}$ coupling. We demonstrate that the angular distribution of the charged lepton from $Z$ boson...

    Go to contribution page
  174. Gonzalo Enrique Orellana (National University of La Plata (AR))
    28/05/2020, 18:45
    Upgrade & Future
    Experimental poster

    ATLAS electron and photon triggers covering transverse energies from 5 GeV to several TeV are essential to record signals for a wide variety of physics: from Standard Model processes to searches for new phenomena. During Run 3 (2021-2024) main triggers used for those physics studies will be a single-electron trigger with ET threshold around 25 GeV and a diphoton trigger with thresholds at 25...

    Go to contribution page
  175. Ms Samadrita Mukherjee (Indian Association for the Cultivation of Science)
    28/05/2020, 18:45
    TeV-Scale BSM
    Theory poster

    Presence of non-holomorphic soft SUSY breaking terms is known to be a possibility in the popular setup of the Minimal Supersymmetric Standard Model (MSSM). It has been shown that such a scenario known as Non-Holomorphic Supersymmetric Standard Model (NHSSM) could remain ‘natural’ (i.e., not fine-tuned) even in the presence of a rather heavy higgsino-like LSP. In a first study of such a...

    Go to contribution page
  176. Mr Zhongyukun Xu (Shandong University (CN))
    28/05/2020, 18:45
    TeV-Scale BSM
    Experimental poster

    A search for heavy resonances decaying into WW, Z Z or W Z using proton–proton collision data at a centre-of-mass energy of √ s = 13 TeV. The data, corresponding to an integrated luminosity of 139 fb−1 , were recorded with the ATLAS detector from 2015 to 2018 at the Large Hadron Collider. The search is performed for final states in which one W or Z boson decays leptonically, and the other W...

    Go to contribution page
  177. Hoang Dai Nghia Nguyen (CPPM, Aix-Marseille Université, CNRS/IN2P3 (FR))
    28/05/2020, 18:45
    TeV-Scale BSM
    Experimental poster

    Events with a large number of high-pT b-jets are rare in the Standard Model (SM); an excess of events with such topology would be a signal of phenomena beyond the SM. One phenomenon where a large excess is expected is a variant of supersymmetry in which R-parity is violated, allowing baryon number violating decays of the super partners of the SM particles.

    This analysis presents the search...

    Go to contribution page
  178. Krisztian Farkas (Eotvos Lorand University (HU))
    28/05/2020, 18:45
    TeV-Scale BSM
    Experimental poster

    Most recent results on searches for supersymmetric (SUSY) particles decaying to final states containing high energy photon(s) are presented. The searches are based on data collected at the center-of-mass energy of 13 TeV in proton-proton collisions recorded by the CMS detector.

    Go to contribution page
  179. Hassnae El Jarrari (Universite Mohammed V (MA))
    28/05/2020, 18:45
    Dark Sector BSM
    Experimental poster

    Many extensions to the Standard Model introduce a hidden or dark
    sector to provide candidates for dark matter in the universe an
    explanation to astrophysical observations such as the positron excess
    observed in the cosmic radiation flux. this hidden sector could rise
    from an additional U(1)d gauge symmetry. The gauge boson of the dark
    sector would be either a massless or a massive dark...

    Go to contribution page
  180. Auriane Canesse (McGill University, (CA))
    28/05/2020, 18:45
    Upgrade & Future
    Experimental poster

    The instantaneous luminosity of the Large Hadron Collider at CERN will be increased by about a factor of five with respect to the design value by undergoing an extensive upgrade program over the coming decade. The largest phase-1 upgrade project for the ATLAS Muon System is the replacement of the present first station in the forward regions with the New Small Wheels (NSWs) during the long-LHC...

    Go to contribution page
  181. Ms Apurba Tiwari (Aligarh Muslim University)
    28/05/2020, 18:45
    TeV-Scale BSM
    Theory poster

    We study new physics contributions to Wtb anomalous couplings in top-quark decay process t-> Wb at the partonic level. In particular, we compute the limits on anomalous couplings to Wtb vertex. Limits were obtained at 13 TeV LHC energy with an integrated luminosity of 36.1 fb^-1 and predictions for future circular colliders, namely, HL-LHC, HE-LHC and FCC-hh were given. For future colliders,...

    Go to contribution page
  182. Ana Luisa Carvalho (LIP (PT))
    28/05/2020, 18:45
    Upgrade & Future
    Experimental poster

    For the High-Luminosity LHC, planned to start in 2027, the ATLAS experiment will be equipped with the Hardware Tracking for the Trigger (HTT) system, a dedicated hardware system able to reconstruct tracks in the silicon detectors with short latency. The evolved TDAQ system design consists of a two-level hardware trigger in which the HTT is used in a low-latency mode (L1Track), providing tracks...

    Go to contribution page
  183. Marco Aparo (University of Sussex (GB))
    28/05/2020, 18:45
    Performance
    Experimental poster

    The Inner Detector (ID) trigger plays an essential role in the ATLAS trigger system, enabling the high purity reconstruction of physics objects - electron, tau, muon, bjet candidates, providing access to regions of the phase space populated by these objects which span a wide range of kinematic regimes. These are essential for the core physics programme at ATLAS: Standard Model measurements;...

    Go to contribution page
  184. Alec Swenson Drobac (Tufts University (US))
    28/05/2020, 18:45
    Performance
    Experimental poster

    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...

    Go to contribution page
  185. Emma Torro Pastor (Univ. of Valencia and CSIC (ES))
    28/05/2020, 18:45
    Performance
    Experimental poster

    The ATLAS experiment aims to record about 1 kHz of physics collisions. This is achieved by using a two-level trigger system to select interesting physics events while reducing the data rate from the 40 MHz LHC crossing frequency. Events are selected based on physics signatures such as the presence of energetic leptons, photons, jets or large missing energy. The wide physics programme carried...

    Go to contribution page
  186. Sebastian Bysiak (Institute of Nuclear Physics Polish Academy of Sciences (PL))
    28/05/2020, 18:45
    Upgrade & Future
    Experimental poster

    In preparation for LHC Run 3 ALICE will upgrade its subsystems to cope with the increased interaction rate of 50 kHz in Pb-Pb and up to 1 MHz in other collision systems, resulting in the data throughput from the detector up to 3 TB/s. Storing and analyzing such amount of data is a significant challenge and therefore, the online event selection will be required.

    The Fast Interaction Trigger...

    Go to contribution page
  187. Solangel Rojas (Czech Technical University (CZ))
    28/05/2020, 18:45
    Upgrade & Future
    Experimental poster

    ALICE (A Large Ion Collider Experiment) is one of the four main detectors at CERN LHC. In order to exploit the increased luminosity and interaction rate during the upcoming LHC Run 3 and 4, ALICE is now implementing a significant upgrade of its detectors and systems.

    The minimum latency interaction trigger, luminosity monitoring, precision collision time, and determination of centrality and...

    Go to contribution page
  188. Di Wang (Tsinghua University (CN))
    28/05/2020, 18:45
    Dark Sector BSM
    Experimental poster

    Although the Standard Model successfully explains most phenomena at the LHC, there are several outstanding questions, including the nature of dark matter, the origin of neutrino masses, and the asymmetry in matter and anti-matter abundances in the Universe. Located in the side tunnel TI12, FASER (Forward Search Experiment) will search for highly displaced signals from light and extremely...

    Go to contribution page
  189. Silvia Franchino (Ruprecht Karls Universitaet Heidelberg (DE))
    28/05/2020, 18:45
    Upgrade & Future
    Experimental poster

    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 is expected to run at higher energy and instantaneous luminosity, L1Calo is currently implementing a significant programme of planned...

    Go to contribution page
  190. Daniel Turgeman (Weizmann Institute of Science (IL))
    28/05/2020, 18:45
    QCD physics
    Experimental poster

    A new method for identifying hints of possible beyond the standard model (BSM) signals with energetic high jet multiplicity final states is proposed. In particular, the QCD background is estimated in a data driven way. Based on the simplified picture where QCD multijet events are created from a 2$\to$2 process followed by cascade branching of the outcoming partons, the proposed “Two...

    Go to contribution page
  191. Simone Ragoni (University of Birmingham (GB))
    28/05/2020, 18:45
    Heavy Ions
    Experimental poster

    Ultraperipheral Collisions (UPC) occur when the interacting nuclei or protons have an impact parameter larger than the sum of their radii. They are mediated by virtual photon exchange. The photoproduction of heavy vector mesons is especially interesting because they couple to the photon.

    The ALICE Collaboration has analysed both p-Pb and Pb--Pb UPC at the centre-of-mass energy of...

    Go to contribution page
  192. Sizar Aziz (Université Paris-Saclay (FR))
    28/05/2020, 18:45
    Heavy Ions
    Experimental poster

    To compute cross sections in proton-proton collisions, parton distribution functions (PDFs) are used which describe the density of partons within the proton. In nuclear environments, such as heavy ions, these densities change and therefore PDFs must be modified to nuclear PDFs (nPDFs). Measurements of electroweak bosons help to constrain the nPDFs. This in turn allows to compute cross sections...

    Go to contribution page
  193. Jinlin Fu (Università degli Studi e INFN Milano (IT))
    29/05/2020, 12:30
  194. Tao Liu (The Hong Kong University of Science and Technology)
    29/05/2020, 12:30
  195. Émilien Chapon (Chinese Academy of Sciences (CN))
    29/05/2020, 12:30
  196. Federico Buccioni (University of Oxford)
    29/05/2020, 12:30
  197. Nan Lu (California Institute of Technology (US))
    29/05/2020, 12:30
  198. Brian Shuve (Harvey Mudd College)
    29/05/2020, 12:30
  199. Till Martini (HU Berlin)
    29/05/2020, 12:30
  200. Luca Rottoli (University of Milan-Bicocca)
    29/05/2020, 12:45
  201. Alberto Bragagnolo (Università e INFN, Padova (IT))
    29/05/2020, 12:48
  202. Kirill Skovpen (Ghent University (BE))
    29/05/2020, 12:48
  203. Nestor Armesto Perez (Universidade de Santiago de Compostela (ES))
    29/05/2020, 12:48
  204. Mr Constantin Niko Weisser (Massachusetts Inst. of Technology (US))
    29/05/2020, 12:48
  205. Oscar Gonzalez Lopez (Centro de Investigaciones Energéti cas Medioambientales y Tecno)
    29/05/2020, 12:48
  206. Heather Russell (McGill University (CA))
    29/05/2020, 12:48
  207. Jonathon Mark Langford (Imperial College (GB))
    29/05/2020, 13:00
  208. Huasheng Shao (Centre National de la Recherche Scientifique (FR))
    29/05/2020, 13:06
  209. Maria Smizanska (Lancaster University (GB))
    29/05/2020, 13:06
  210. Michaela Queitsch-Maitland (CERN)
    29/05/2020, 13:06
  211. Miaoran Lu (University of Science and Technology of China (CN))
    29/05/2020, 13:06
  212. Mariarosaria D'Alfonso (Massachusetts Inst. of Technology (US))
    29/05/2020, 13:06
  213. Paolo Sabatini (Georg August Universitaet Goettingen (DE))
    29/05/2020, 13:13
  214. Nikita Belyaev (National Research Nuclear University MEPhI (RU))
    29/05/2020, 13:15
  215. Mr Pantelis Kontaxakis (National and Kapodistrian University of Athens (GR))
    29/05/2020, 13:24
  216. Mykola Khandoga (Université Paris-Saclay (FR))
    29/05/2020, 13:24
  217. Dr Vasiliki Mitsou (Univ. of Valencia and CSIC (ES))
    29/05/2020, 13:24
  218. Jana Crkovska (Los Alamos National Laboratory (US))
    29/05/2020, 13:24
  219. Christoph Bobeth (Technical University Munich)
    29/05/2020, 13:24
  220. Shankha Banerjee (University of Durham (GB))
    29/05/2020, 13:30
  221. Nicolas Pierre Chanon (Centre National de la Recherche Scientifique (FR))
    29/05/2020, 13:31
  222. Daniel Stolarski (Carleton University (CA))
    29/05/2020, 14:15
    Talk
  223. Meirin Oan Evans (University of Sussex (GB))
    29/05/2020, 14:15
    Outreach
    Talk
  224. Alessio Tiberio (Universita e INFN, Firenze (IT))
    29/05/2020, 14:15
  225. Francisco Yumiceva (Florida Institute of Technology (US))
    29/05/2020, 14:15
  226. Liupan An (Universita e INFN, Firenze (IT))
    29/05/2020, 14:15
  227. Cristina Terrevoli (University of Houston (US))
    29/05/2020, 14:33
  228. Merve Nazlim Agaras (Université Clermont Auvergne (FR))
    29/05/2020, 14:33
  229. Ian Dyckes (University of Pennsylvania (US))
    29/05/2020, 14:33
    Talk
  230. Herbi Dreiner (Bonn University)
    29/05/2020, 14:33
    Outreach
    Talk
  231. Francesco Cafagna (Universita e INFN, Bari (IT))
    29/05/2020, 14:33
  232. Mariia Savina (Joint Institute for Nuclear Research (RU))
    29/05/2020, 14:51
    Talk
  233. Stefanos Leontsinis (Universitaet Zuerich (CH))
    29/05/2020, 14:51
  234. Joshuha Thomas-Wilsker (Institute Of High Energy Physics, Beijing)
    29/05/2020, 14:51
  235. Ivica Puljak (University of Split. Fac.of Elect. Eng., Mech. Eng. and Nav.Arc)
    29/05/2020, 14:51
    Outreach
    Talk
  236. Ameir Shaa Bin Akber Ali (Nanyang Technological University (SG))
    29/05/2020, 14:51
  237. Zhen Hu (Tsinghua University (CN))
    29/05/2020, 15:09
  238. Dr Peter Galler (University of Glasgow)
    29/05/2020, 15:09
  239. Marek Karliner (Tel Aviv University (IL)), Marek Karliner (Tel Aviv University (IL))
    29/05/2020, 15:09
  240. Laura Molina Bueno (ETH Zurich (CH))
    29/05/2020, 15:09
    Talk
  241. Ioannis Tsinikos (LU)
    29/05/2020, 15:27
  242. Wolfgang Altmannshofer (UC Santa Cruz)
    29/05/2020, 16:00
  243. Augusto Ceccucci (CERN)
    29/05/2020, 16:30
  244. Maurizio Martinelli (Universita & INFN, Milano-Bicocca (IT))
    29/05/2020, 17:00
  245. Mark Peter Whitehead (University of Bristol (GB))
    29/05/2020, 17:30
  246. Giacomo Fedi (Imperial College (GB))
    29/05/2020, 18:00
  247. Simon Knapen (CERN)
    30/05/2020, 12:30
    Talk
  248. Katherine Pachal (Duke University (US))
    30/05/2020, 13:00
    Talk
  249. Bhawna Gomber (University of Hyderabad, India)
    30/05/2020, 13:30
    Talk
  250. Chris Quigg (Fermi National Accelerator Lab. (US)), Greg Landsberg (Brown University (US)), Jan Fiete Grosse-Oetringhaus (CERN), Marjorie Shapiro (Lawrence Berkeley National Lab. (US)), Monica Pepe-Altarelli (CERN)
    30/05/2020, 14:15
  251. Tamas Almos Vami (Johns Hopkins University (US))
    30/05/2020, 14:30
  252. Despina Hatzifotiadou (Universita e INFN, Bologna (IT))
    30/05/2020, 14:45
  253. Eckhard Elsen (CERN)
    30/05/2020, 15:00
  254. Beniamino Di Girolamo (CERN)
    30/05/2020, 15:30
  255. Andreas Hoecker (CERN)
    30/05/2020, 15:55
  256. Bruno Mansoulie (Université Paris-Saclay (FR)), Tulika Bose (University of Wisconsin Madison (US))
    30/05/2020, 16:35
  257. Talk

    physics motivation and challenges, timeline, costs, design

    Go to contribution page