26 September 2021 to 1 October 2021
Europe/Rome timezone

Contribution List

101 out of 101 displayed
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  1. Angelo Scribano Memoria (Universita & INFN Pisa (IT)), Christophe Royon (The University of Kansas (US))
    27/09/2021, 14:00
  2. Jamal Jalilian-Marian (Baruch College)
    27/09/2021, 14:10
  3. Amanda Sarkar (University of Oxford (GB)), amanda sarkar
    27/09/2021, 14:30
  4. Cristina Sánchez Gras (Nikhef National institute for subatomic physics (NL))
    27/09/2021, 14:55
  5. Toni Makela (Deutsches Elektronen-Synchrotron (DE))
    27/09/2021, 15:20
  6. Nicola Neri (Università degli Studi e INFN Milano (IT))
    27/09/2021, 16:10
  7. Tomasz Stebel (Institute of Theoretical Physics Jagiellonian University), Tomasz Stebel (CERN)
    27/09/2021, 16:30
  8. Zhiqing Philippe Zhang (IJCLab, Orsay (FR))
    27/09/2021, 16:50
  9. Thomas Chen (Academy for Mathematics, Science, and Engineering)
    27/09/2021, 17:15
  10. Stanley J. Brodsky (SLAC National Accelerator Laboratory, Stanford University)
    27/09/2021, 17:35
  11. Cyrille Marquet (CPHT - Ecole Polytechnique), Dimitri Colferai (University of Florence), Krzysztof Kutak (Instytut Fizyki Jadrowej Polskiej Akademii Nauk)
    27/09/2021, 18:00
  12. Salim Cerci (Adiyaman University (TR) - Istanbul University (TR))
    28/09/2021, 09:00
  13. Michael Lublinsky (Ben-Gurion University of the Negev (IL))
    28/09/2021, 09:25
  14. Grigorios Chachamis (LIP, Lisbon)
    28/09/2021, 09:45
  15. Federico Deganutti
    28/09/2021, 10:05
  16. Dimitri Colferai (University of Florence)
    28/09/2021, 10:25
  17. Irais Bautista Guzman (Centro de Investigación y de Estudios Avanzados del IPN (MX))
    28/09/2021, 11:10
  18. Francesco Giovanni Celiberto (Università della Calabria and INFN Cosenza (Italy)), Francesco Giovanni Celiberto (ECT*/FBK Trento & INFN-TIFPA)
    28/09/2021, 11:30
  19. Leszek Motyka
    28/09/2021, 11:50
  20. Yoshitaka Itow
    28/09/2021, 12:10
  21. Cyrille Marquet (CPHT - Ecole Polytechnique), Dimitri Colferai (University of Florence), Krzysztof Kutak (Instytut Fizyki Jadrowej Polskiej Akademii Nauk)
    28/09/2021, 12:35
  22. Cyrille Marquet (CPHT - Ecole Polytechnique)
    28/09/2021, 14:30
  23. Yair Mulian
    28/09/2021, 14:50
  24. Tanguy Pierog (KIT)
    28/09/2021, 15:10
  25. Krzysztof Kutak (Instytut Fizyki Jadrowej Polskiej Akademii Nauk)
    28/09/2021, 15:35
  26. Cristian Baldenegro Barrera (The University of Kansas (US))
    28/09/2021, 15:55
  27. Marco Santimaria (INFN e Laboratori Nazionali di Frascati (IT)), Marco Santimaria
    28/09/2021, 16:40
  28. Deniz Sunar Cerci (Adiyaman University (TR) - Istanbul University (TR))
    28/09/2021, 17:05
  29. Francesco Giuli (INFN e Universita Roma Tor Vergata (IT))
    28/09/2021, 17:30
  30. Ben Nachman (Lawrence Berkeley National Lab. (US))
    28/09/2021, 17:55
  31. Cyrille Marquet (CPHT - Ecole Polytechnique), Dimitri Colferai (University of Florence), Krzysztof Kutak (Instytut Fizyki Jadrowej Polskiej Akademii Nauk)
    28/09/2021, 18:20
  32. Frigyes Janos Nemes (CERN (also at Wigner RCP Budapest, Hungary))
    29/09/2021, 09:00
  33. Carlos Arturo Avila Bernal (Universidad de los Andes), Carlos Avila Bernal (Universidad de los Andes (CO))
    29/09/2021, 09:20
  34. Tamas Csorgo (Wigner Research Centre for Physics (Wigner RCP) (HU))
    29/09/2021, 09:40
  35. Vladimir Petrov (Institute for High Energy Physics of NRC Kurchatov Institute (R), Vladimir Petrov, Vladimir Petrov (Joint Institute for Nuclear Research (JINR)), Vladimir Petrov
    29/09/2021, 10:00
  36. Istvan Szanyi (Hungarian Academy of Sciences (HU)), István Szanyi (Eötvös Loránd University)
    29/09/2021, 10:20
  37. Kenneth Osterberg (University of Helsinki), Kenneth Osterberg (Helsinki Institute of Physics (FI))
    29/09/2021, 10:40
  38. Lucian Harland-Lang (University of Oxford)
    29/09/2021, 11:20
  39. Michael Albrow (Fermi National Accelerator Lab. (US))
    29/09/2021, 11:40
  40. Dmitry Melnikov (Rutgers University)
    29/09/2021, 12:00
  41. Mark Strikman, Mark Strikman (Penn State University), Mark Strikman (Pennsylvania State University (US))
    29/09/2021, 12:20
  42. Christophe Royon (The University of Kansas (US)), Kenneth Osterberg (University of Helsinki), Kenneth Osterberg (Helsinki Institute of Physics (FI))
    29/09/2021, 12:40
  43. Georgios Krintiras (The University of Kansas (US))
    30/09/2021, 09:00
  44. Thomas Boettcher (University of Cincinnati (US)), Thomas Julian Boettcher (University of Michigan (US))
    30/09/2021, 09:25
  45. Jens Robert Luhder (Westfaelische Wilhelms-Universitaet Muenster (DE))
    30/09/2021, 09:50
  46. Luis Alcerro Alcerro (The University of Kansas (US))
    30/09/2021, 10:15
  47. Weisong Duan (South China Normal University (CN)), Weisong Duan (South China Normal University)
    30/09/2021, 11:00
  48. Laura Fabbri (Universita e INFN, Bologna (IT))
    30/09/2021, 11:25
  49. Vieri Candelise (Universita di Roma I "La Sapienza"-Universita & INFN, Roma I), Vieri Candelise (Universita e INFN Trieste (IT))
    30/09/2021, 11:50
  50. Despoina Sampsonidou (Tsung-Dao Lee Institute (CN) & Shanghai Jiao Tong Univ. (CN))
    30/09/2021, 12:15
  51. Georgios Krintiras (The University of Kansas (US)), Irais Bautista Guzman (Centro de Investigación y de Estudios Avanzados del IPN (MX))
    30/09/2021, 12:40
  52. Mario Deile (CERN), Mario Deile (CERN)
    30/09/2021, 14:30
  53. Maciej Piotr Lewicki (Polish Academy of Sciences (PL))
    30/09/2021, 14:55
  54. Christophe Royon (The University of Kansas (US))
    30/09/2021, 15:20
  55. Andrea Bellora (Universita e INFN Torino (IT))
    30/09/2021, 15:40
  56. Cristian Baldenegro Barrera (The University of Kansas (US))
    30/09/2021, 16:00
  57. Michael Pitt (CERN)
    30/09/2021, 16:25
  58. Ada Solano (Universita' di Torino e INFN (IT))
    30/09/2021, 17:10
  59. Beatriz Ribeiro Lopes (Deutsches Elektronen-Synchrotron (DE))
    30/09/2021, 17:35
  60. Krzysztof Cieśla (Polish Academy of Sciences (PL))
    30/09/2021, 18:00
  61. Maciej Trzebinski (Polish Academy of Sciences (PL))
    30/09/2021, 18:25
  62. Leszek Motyka, Mario Deile (CERN), Michael Albrow (Fermi National Accelerator Lab. (US)), Valentina Avati (AGH University of Science and Technology (PL))
    30/09/2021, 18:45
  63. Daniel Camarero Munoz (Universidad Autonoma de Madrid (ES))
    01/10/2021, 09:00
  64. Marta Ruspa (Universita e INFN Torino (IT))
    01/10/2021, 09:25
  65. Simone Ragoni (University of Birmingham (GB))
    01/10/2021, 09:50
  66. Antoni Szczurek (Institute of Nuclear Physics)
    01/10/2021, 10:15
  67. Piotr Lebiedowicz (Institute of Nuclear Physics PAN)
    01/10/2021, 10:35
  68. Barbara Linek, Marta Luszczak (University of Rzeszow)
    01/10/2021, 11:20
  69. Mohammed Maher Abdelrahim Mohammed (University of Calabria and INFN - Gruppo collegato di Cosenza)
    01/10/2021, 11:40
  70. Spencer Robert Klein (Lawrence Berkeley National Lab. (US))
    01/10/2021, 12:00
  71. Georgios Krintiras (The University of Kansas (US)), Irais Bautista Guzman (Centro de Investigación y de Estudios Avanzados del IPN (MX))
    01/10/2021, 12:25
  72. Angelo Scribano Memoria (Universita & INFN Pisa (IT)), Christophe Royon (The University of Kansas (US))
    01/10/2021, 12:55
  73. Barbara Badelek (University of Warsaw (PL))
  74. Irais Bautista Guzman (Centro de Investigación y de Estudios Avanzados del IPN (MX))

    We use a two-function interplay model parametrization to describe data of the pp cross-section by the increase of matter density to the black disk saturation limit and the radial expansion through the growth of the overlap area based on a geometric scaling model. We argue two mechanisms responsible for the growth of high energy cross-sections in pp collisions by using data on different species...

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  75. Sebastian Neubert (University of Bonn (DE))

    In 2018, LHCb recorded $\sim 210 \mu b^{-1}$ integrated luminosity of PbPb
    collisions at $\sqrt{s_{NN}}$ = 5.02 TeV. With an increase of the luminosity by a
    factor 20 compared to the previous 2015 PbPb dataset, precise measurements on
    photo-produced charmonia in ultra-peripheral collisions are foreseen. Moreover,
    the great momentum resolution of the detector allows to study...

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  76. Nicola Neri (Università degli Studi e INFN Milano (IT))

    Magnetic and electric dipole moments of fundamental particles provide powerful probes for physics within and beyond the Standard Model. For the case of short-lived particles these have not been experimentally accessible to date due to the difficulties imposed by their short lifetimes. A unique program of direct measurements of electromagnetic dipole moments of strange and charm baryons, and...

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  77. Dr Lucian Harland-Lang (University of Oxford)

    We discuss the role of additional hadron-hadron interactions in elastic photon-initiated production at the LHC, both in proton and heavy ion collisions. We in particular assess different sources of uncertainty associated with these cross sections, and compare with other calculations in the literature. A key result of our analysis is that the uncertainty associated with the survival factor is...

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  78. Agustin Sabio Vera, Agustin Sabio Vera
  79. Yair Mulian

    Using the CGC effective theory together with the hybrid factorisation, we study forward dijet production in proton-nucleus collisions beyond leading order. In this paper, we compute the "real" next-to-leading order (NLO) corrections, i.e. the radiative corrections associated with a three-parton final state, out of which only two are being measured. To that aim, we start by revisiting our...

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  80. Prof. Mark Strikman (Penn State University)

    We review a number of coherent phenomena which are studied in the ultraperipheral collisions (UPC) at the LHC. In particular, we demonstrate that much larger shadowing for coherent rho-meson production than in the Glauber model naturally emerges in the color fluctuation picture of high energy hadron – nucleon interaction. We also demonstrate that the theory of the leading twist gluon...

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  81. Maciej Trzebinski (Polish Academy of Sciences (PL))

    Diffractive processes possible to be measured at the LHC will be briefly discussed. This includes soft (elastic scattering, exclusive meson pair production, diffractive bremsstrahlung) and hard (single and double Pomeron exchange jets, γ+jet, W/Z, jet-gap-jet, exclusive jets) processes as well as Beyond Standard Model phenomena (anomalous gauge couplings, magnetic monopoles).

    Feasibility...

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  82. Mohammed Maher Abdelrahim Mohammed (Università della Calabria & INFN-Cosenza)

    We present recent BFKL phenomenological results for the inclusive production of a Higgs in association with a jet, as a testfield for the semi-hard regime of QCD. We show how the large energy scales provided by the emission of a Higgs boson stabilize the BFKL series, and discuss the possible extension of this work in the full NLA BFKL analysis, by including the NLO jet impact factor, with a...

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  83. Tomasz Stebel (Jagiellonian University)

    High multiplicity events in small collision systems ($pp$ and $pA$ collisions) at hadron colliders have received much attention in recent years. In this talk we will present analysis of $J/\psi$ polarization in high multiplicity hadron collisions using the CGC+NRQCD framework. Predictions both for $pp$ and $pA$ at LHC energies will be presented.

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  84. Collaboration H1 (DESY)

    Recently, jet measurements in DIS events close to Born kinematics have been proposed as a new probe to study transverse-momentum-dependent (TMD) PDFs, TMD fragmentation functions, and TMD evolution. We report measurements of lepton-jet momentum imbalance and hadron-in-jet correlations in high-$Q62$ DIS events collected with the H1 detector at HERA. The jets are reconstructed with the kT...

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  85. Collaboration H1 (DESY)

    A first measurement of the 1-jettiness event shape observable in neutral-current deep-inelastic electron-proton scattering is presented. The 1-jettiness observable $\tau_{1b}$ is defined such that it is equivalent to the thrust observable in the Breit frame, following momentum conservation. The data were taken with the H1 detector at the HERA $ep$ collider at a center-of-mass energy of 319 GeV...

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  86. Collaboration H1 (DESY)

    Charged particle multiplicity distributions in positron-proton deep inelastic scattering at a centre-of-mass energy $\sqrt{s}=319$ GeV are measured. The data are collected with the H1 detector at HERA corresponding to an integrated luminosity of 136 pb$^{−1}$. Charged particle multiplicities are measured as a function of photon virtuality $Q^2$, inelasticity $y$ and pseudorapidity $\eta$ in...

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  87. Collaboration H1 (DESY)

    Exclusive photoproduction of $\rho^0(770)$ mesons is studied using the H1 detector at the $ep$ collider HERA. A sample of about 900000 events is used to measure single- and double-differential cross sections for the reaction $\gamma p\to \pi^{+}\pi^{-}Y$. Reactions where the proton stays intact ($m_Y=m_p$) are statistically separated from those where the proton dissociates to a low-mass...

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  88. Krzysztof Kutak (Instytut Fizyki Jadrowej Polskiej Akademii Nauk)

    I would like to present recently obtained results for distribution of soft gluons that are produced by hard jet propagating through quark gluon plasma.
    The results are based on the papers:
    https://link.springer.com/article/10.1007/JHEP04(2021)014
    https://journals.aps.org/prc/abstract/10.1103/PhysRevC.102.044910

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  89. Federico Deganutti

    We present, the results of a phenomenology analysis at Next-to-Leading accuracy for the Mueller-Tang jet process, where two jets separated by a large rapidity interval and no other radiation are observed. This process is of high interest, as one might be able to investigate Balitsky-Fadin-Kuraev-Lipatov (BFKL) dynamics which emerges in the high-energy limit of quantum chromodynamics...

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  90. LHCb Collaboration

    LHCb is a spectrometer that covers the forward region of proton-proton collisions, in the pseudo-rapidity range from 2 to 5. At LHCb, proton Parton Distribution Functions (PDFs) can be studied in a unique phase space complementary to that accessible by ATLAS and CMS, corresponding to low and high Bjorken-x. In this talk, the measurements of vector boson production in the forward region, with...

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  91. Toni Makela (Deutsches Elektronen-Synchrotron (DE))

    Jet production is an important probe of both QCD and new physics. Recent CMS measurements involving jet production are presented. In particular, the CMS 13 TeV inclusive jet data are used in a QCD analysis together with HERA inclusive deep inelastic scattering and CMS 13 TeV triple-differential top quark-antiquark pair production cross sections. The parton distributions and the strong coupling...

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  92. Simone Ragoni (University of Birmingham (GB))

    Simone Ragoni$^1$, on behalf of the ALICE Collaboration

    $^1$ University of Birmingham, Birmingham, B15 2TT, UK
    simone.ragoni@cern.ch

    Ultra-peripheral collisions (UPC) are events characterised by large impact parameters between the two projectiles, larger than the sum of their radii. As a consequence, the protons and ions accelerated by the LHC are beyond the reach of the strong...

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  93. Collaboration H1 (DESY)

    Measurements of two- and multi-particle angular correlations in DIS and photoproduction ep collisions at $\sqrt{s}=319$ GeV are presented as a function of charged particle multiplicity. The data were collected using the H1 detector at HERA. Since no long-range ridge structure is observed in the correlation functions over the full multiplicity range, upper limits of ridge yield are provided as...

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  94. Thomas Chen (Academy for Mathematics, Science, and Engineering)

    Recent research by CERN has revealed machine learning-driven capabilities for the identification of proton-proton collisions at LHC for reanalysis. While this work and other previous works also work on speeding up inference via the machine learning algorithm, in this work we propose harnessing Hadamard matrices for faster inference at the model level. Machine learning algorithms for...

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  95. Ronan Mcnulty (University College Dublin (IE))
  96. Pasquale Di Nezza (INFN e Laboratori Nazionali di Frascati (IT))

    The goal of LHCspin is to develop, in the next few years, innovative solutions and cutting-edge technologies to access spin physics in high-energy polarized fixed-target collisions, by exploring a unique kinematic regime given by the LHC beam and by exploiting new probes.
    This ambitious task poses its basis on the recent installation of SMOG2, the unpolarized gas target in front of the LHCb...

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  97. Leszek Motyka

    We perform a twist decomposition of the proton structure functions that evolve according to the Balitsky-Kovchegov equation at the LL order. Using the Mellin space technique we isolate the linear (BFKL) effects and the non-linear (BK) corrections for the leading and subleading twist contributions.

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  98. Jochen Bartels