Contribution List

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  1. 18/05/2026, 08:45
  2. Georges Trad (CERN)
    18/05/2026, 09:00
  3. Paula Collins (CERN)
    18/05/2026, 09:30
  4. Nima Zardoshti (CERN)
    18/05/2026, 10:00
  5. Anna Sfyrla (Universite de Geneve (CH))
    18/05/2026, 11:00
  6. Filip Moortgat (CERN)
    18/05/2026, 11:30
  7. Sara Garetti (Université Paris-Saclay (FR))
    18/05/2026, 12:00
  8. David Barney (CERN)
    18/05/2026, 12:15
  9. Dilia Maria Portillo Quintero (TRIUMF (CA))
    18/05/2026, 12:30
  10. Argyro Ziaka (University of Ioannina (GR))
    18/05/2026, 14:00
  11. Bartlomiej Henryk Zabinski (Polish Academy of Sciences (PL))
    18/05/2026, 14:00
  12. Pedro Fernandez Manteca (CERN)
    18/05/2026, 14:00

    The presentation focuses on complete LHC Run2 results, including combinations of various channels - CMS speaker (15' presentation + 3' discussion)

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  13. Nathan Grieser (University of Cincinnati (US))
    18/05/2026, 14:00
  14. Federica Primavera (Universita e INFN, Padova (IT))
    18/05/2026, 14:18
  15. Yanping Huang (Chinese Academy of Sciences (CN)), Yanping Huang (Chinese Academy of Sciences (CN))
    18/05/2026, 14:18

    LHC Run3 results focus, including updates on Run 3 physics objects reconstruction, identification & dedicated triggers - ATLAS speaker (15' presentation + 3' discussion)

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  16. Jan Eysermans (Massachusetts Inst. of Technology (US))
    18/05/2026, 14:18
  17. Mark Hodgkinson (University of Sheffield (GB))
    18/05/2026, 14:18
  18. MATTEO MARCOLI (University of Durham)
    18/05/2026, 14:18
  19. Wenhao Ma (University of Science and Technology of China (CN))
    18/05/2026, 14:36
  20. Fabio Colamaria (INFN, Sezione di Bari (IT))
    18/05/2026, 14:36
  21. Hugues Evard (Universite Libre de Bruxelles (BE))
    18/05/2026, 14:36
  22. Ryan Roberts (University of Chicago (US))
    18/05/2026, 14:36

    Including EFT and anomalous couplings interpretations - ATLAS speaker (15' presentation + 3' discussion)

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  23. Dr Daniil Ponomarenko (Indiana University (US))
    18/05/2026, 14:36
  24. Marco Menen, Marco Menen (Leibniz Universität Hannover)
    18/05/2026, 14:54

    15' presentation + 3' discussion

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  25. Renato Quagliani (CERN)
    18/05/2026, 14:54
  26. Thomas Cridge (DESY)
    18/05/2026, 14:54
  27. Yang Liu (Sun Yat-Sen University (CN))
    18/05/2026, 14:54
  28. Jack Holguin
    18/05/2026, 14:54
  29. Paul Gaigne (Université Paris-Saclay (FR))
    18/05/2026, 15:09

    15' presentation + 3' discussion - CMS speaker

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  30. Manuel Ramirez Garcia (University of Michigan (US))
    18/05/2026, 15:12
  31. Halil Saka (University of Cyprus (CY))
    18/05/2026, 15:12
  32. Volodymyr Svintozelskyi (Univ. of Valencia and CSIC (ES))
    18/05/2026, 15:12
  33. Stefano Manzoni (CERN)
    18/05/2026, 16:00
  34. Xiaohu Sun (Peking University (CN))
    18/05/2026, 16:24
  35. Mr Xuhao Yuan (Institute of High Energy Physics, Beijing, China)
    18/05/2026, 16:48
  36. Antonio Di Mauro (CERN)
    18/05/2026, 17:12
  37. Mark Thomson (CERN)
    18/05/2026, 17:36
  38. Roberto Franceschini (Rome 3 U.)
    19/05/2026, 09:00
  39. Karri Folan Di Petrillo (University of Chicago)
    19/05/2026, 09:30
  40. Daniel Hayden (Michigan State University (US))
    19/05/2026, 10:00
  41. Vit Kucera (Inha University (KR))
    19/05/2026, 11:00
  42. Aritra Bal (KIT - Karlsruhe Institute of Technology (DE))
    19/05/2026, 11:00
  43. Jelle Groot
    19/05/2026, 11:00
  44. Marco Cipriani (Universita & INFN Pisa (IT))
    19/05/2026, 11:00
  45. Ruth Amella Ranz (Centre National de la Recherche Scientifique (FR))
    19/05/2026, 11:00
  46. Zewen Chen (University of Chinese Academy of Sciences (CN))
    19/05/2026, 11:15
  47. Andrew Larkoski (American Physical Society)
    19/05/2026, 11:15
  48. Luke Grazette (University of Warwick (GB))
    19/05/2026, 11:18
  49. Pablo Sesma (IFAE)
    19/05/2026, 11:18
  50. Francesca Carnesecchi (Universita e INFN, Bologna (IT))
    19/05/2026, 11:18
  51. Zackary Lee Alegria (Oklahoma State University (US))
    19/05/2026, 11:30
  52. Lanxing Li (The University of Manchester (GB))
    19/05/2026, 11:30
  53. John Patrick Mc Gowan (University of Victoria (CA))
    19/05/2026, 11:36
  54. Falk Bartels (Heidelberg University (DE))
    19/05/2026, 11:36
  55. Dr Richard Bates (University of Glasgow (GB))
    19/05/2026, 11:36
  56. Vladimir Sergeychik (Tsinghua University (CN))
    19/05/2026, 11:45
  57. Silvia Zanoli (University of Oxford)
    19/05/2026, 11:45
  58. Jannicke Pearkes (University of Colorado Boulder (US))
    19/05/2026, 11:54
  59. Tobias Neumann (William & Mary)
    19/05/2026, 11:54
  60. Mostafa Mahmoud Cherif (Université Paris-Saclay (FR))
    19/05/2026, 11:54
  61. Arne Christoph Reimers (CERN)
    19/05/2026, 12:00
  62. Kylian Demory
    19/05/2026, 12:00
  63. Simone Devoto (Universiteit Gent)
    19/05/2026, 12:12
  64. Nicholas Luongo (Argonne National Laboratory (US))
    19/05/2026, 12:12
  65. Louis D'Eramo (LPCA - CNRS/IN2P3 (FR))
    19/05/2026, 12:12
  66. Nathan Philip Jurik (CERN)
    19/05/2026, 12:15
  67. Qundong Han (Universita e INFN, Padova (IT))
    19/05/2026, 12:15
  68. Francesca Ercolessi (Universita e INFN, Bologna (IT))
    19/05/2026, 14:00
  69. Song-Ming Wang (Academia Sinica (TW))
    19/05/2026, 14:00

    Focusing on the novel techniques and performance in LHC Run3, with perspectives for HL-LHC - ATLAS speaker (15' presentation + 3' discussion)

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  70. Zhuolin Zhang (Shandong University (CN))
    19/05/2026, 14:00
  71. Antonello Polosa
    19/05/2026, 14:00
  72. Shuang Zheng (Peking University (CN))
    19/05/2026, 14:15
  73. Tuba Gundem (Goethe University Frankfurt (DE))
    19/05/2026, 14:18
  74. Giovanni Celotto (University of Zurich (CH))
    19/05/2026, 14:18

    Focusing on the novel techniques and performance in LHC Run3, with perspectives for HL-LHC - CMS speaker (15' presentation + 3' discussion)

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  75. Dr Tanguy Pierog
    19/05/2026, 14:18
  76. Ruobing Jiang (Peking University (CN))
    19/05/2026, 14:21
  77. Semen Turchikhin (INFN e Universita Genova (IT))
    19/05/2026, 14:30
  78. Leszek Adamczyk (AGH University of Science and Technology (PL))
    19/05/2026, 14:36
  79. Davide Zuliani (Universita e INFN, Padova (IT))
    19/05/2026, 14:36

    Focusing on the novel techniques and performance in LHC Run3, with perspectives for HL-LHC - LHCb speaker (15' presentation + 3' discussion)

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  80. Francesco Terzuoli (Università di Siena & INFN Pisa (IT))
    19/05/2026, 14:36
  81. Ken Mimasu (University of Southampton)
    19/05/2026, 14:42
  82. Jhovanny Andres Mejia Guisao (Centro Invest. Estudios Avanz. IPN (MX)), Jhovanny Andres Mejia Guisao (Cinvestav)
    19/05/2026, 14:45
  83. Brunella D'Anzi (Univ. of California San Diego (US))
    19/05/2026, 14:54
  84. Rebecca von Kuk (Univerisity of Bern)
    19/05/2026, 14:54

    15' presentation + 3' discussion

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  85. Gregory Soyez (IPhT, CEA Saclay)
    19/05/2026, 14:54
  86. Antonio Palasciano (Politecnico & INFN, Bari (IT))
    19/05/2026, 15:00
  87. Doreen Wackeroth
    19/05/2026, 15:03
  88. Javier Llorente Merino (CIEMAT - Centro de Investigaciones Energéticas Medioambientales y Tec. (ES))
    19/05/2026, 15:12
  89. Wahid Redjeb (CERN)
    19/05/2026, 15:12
  90. Andrea Tavira (University of Texas at Austin (US))
    19/05/2026, 15:15
  91. Gauthier Legras (Universität Münster (DE))
    19/05/2026, 15:30

    Quarkonia -- bound states of heavy quark-antiquark pairs (charm or bottom) -- offer a unique probe of both perturbative and non-perturbative QCD. While the hard-scale production of the quark-antiquark pairs is calculable via perturbation theory, their hadronization into bound states requires non-perturbative models like NRQCD. In hadronic collisions, the underlying event activity, usually...

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  92. Cristina Alexe (Scuola Normale Superiore & INFN Pisa (IT))
    19/05/2026, 15:31

    We consider a common situation in High Energy Physics (HEP) analyses: performing a maximum-likelihood fit of a physics model to a binned data set with high-statistics, with the goal of setting confidence intervals on a parameter of interest in the presence of systematic uncertainties modeled as nuisance parameters. We focus on the case when the physics model is determined from Monte Carlo (MC)...

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  93. Ali Garabaglu (University of Washington (US))
    19/05/2026, 15:32

    The decay of the Higgs boson into a pair of tau leptons offers direct insight into the Yukawa coupling hierarchy of the Standard Model. Probing this process in the high transverse momentum regime ($p_T$ > 300 GeV) is critical for constraining new physics, yet standard resolved reconstruction algorithms struggle to resolve the increasingly collimated decay products. We presents the first ATLAS...

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  94. Lang Xu (Institute of Particle Physics, CCNU (CN); Institute of physics of 2 infinities of Lyon, UCBL (FR))
    19/05/2026, 15:33

    The enhancement of the strange baryon-to-meson yield ratio at intermediate transverse momentum ($p_{\rm T}$) observed by ALICE across small to large collision systems is usually considered to be driven by collective radial flow and quark recombination effects. Nevertheless, it remains under discussion whether jet fragmentation also contributes to the observed enhancement, as strange particles...

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  95. Dr RAFIQUL RAHAMAN (Institute of Physics, University of Sao Paulo)
    19/05/2026, 15:34

    The non-resonant production of a Higgs boson pair in association with a top–antitop quark pair ($pp \to t\bar{t}hh$) has only recently begun to be explored at the Large Hadron Collider and provides a unique and largely uncharted probe of the top–Higgs sector, offering complementary sensitivity to the Higgs self-coupling and higher-dimensional interactions beyond the Standard Model. In this...

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  96. Songshaptak De (Jožef Stefan Institute)
    19/05/2026, 15:35

    The search for heavy $W'$ bosons in their decay modes to a lepton and a heavy neutrino offers a promising avenue for probing new physics beyond the Standard Model. This work focuses on such a signature with an energetic lepton plus a fat jet, originating from the heavy neutrino and containing a lepton. We have employed the jet substructure techniques to isolate the embedded lepton as a subjet...

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  97. Abhishek Kumar Singh, Abhishek Kumar Singh (Indian Institute Of Technology Delhi)
    19/05/2026, 15:36

    We propose a new collider signature for the composite origin of the electroweak symmetry breaking of the standard model. The Higgs sector consists of new fundamental fermions (hyper-quarks), which confine at a hadronization scale $\Lambda_{HC} \sim$ few TeV. At energies above $\Lambda_{HC}$, the Drell-Yan production of the hyper-quarks leads to the production of a few electroweak bosons, in...

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  98. Alessandro Montella (Stockholm University (SE))
    19/05/2026, 15:37

    Algorithms to identify jets from b-hadrons (b-jets) are widely in use in ATLAS and are crucial for measurements and searches targeting processes with top quarks or Higgs bosons in the final state, for instance, b-tagging played a central role in the observation of the Higgs boson decay into bottom quarks. These b-tagging algorithms are trained on simulation, therefore, their performance in...

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  99. Olivier Salin (Université Paris-Saclay)
    19/05/2026, 15:38

    The High-Luminosity LHC is set to begin operations for physics around 2030, enabling the collection of ten times more data than will have been accumulated by the LHC. The resulting increase in pile-up, radiation exposure, and data volume requires a comprehensive upgrade of both the on‑detector and off‑detector electronics of the ATLAS Liquid Argon (LAr) Calorimeter to maintain excellent energy...

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  100. Shubham Gupta (Brandeis University (US))
    19/05/2026, 15:39

    The ATLAS experiment is currently preparing for an upgrade of the Inner Tracking for High-Luminosity LHC operation, scheduled to start in 2030. The radiation damage at the maximum integrated luminosity of 4000/fb implies integrated hadron fluencies over 2x1016neq/cm2 and tracking in a very dense environment call for a replacement of the existing Inner Detector. An all-silicon Inner Tracker...

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  101. Yuliia Maidannyk (Université Paris-Saclay (FR))
    19/05/2026, 15:40

    Accurate clustering of electromagnetic energy deposits is essential for reconstructing photons and electrons in modern hadron collider experiments, where boosted topologies and pileup often cause overlapping showers and ambiguous energy assignment. We present deep learning-based clustering approaches that reconstruct particle energy and impact position directly from calorimeter readout. The...

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  102. Prof. Anju Bhasin (University of Liverpool)
    19/05/2026, 15:41

    (For ALICE Collaboration)

    Understanding the origin of strangeness enhancement in high-energy hadronic collisions remains one of the central open questions in particle production at the Large Hadron Collider (LHC). Measurements in small collision systems, such as proton–proton (pp) and proton–lead (p–Pb), have revealed striking features traditionally associated with heavy-ion collisions,...

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  103. Kacper Zajac (AGH University of Krakow)
    19/05/2026, 15:42

    Light-by-light scattering is a pure quantum electrodynamic process that proceeds via virtual charged-particle loops, where two photons interact with each other producing another pair of photons. The process was measured for the first time directly in ultra-peripheral Pb+Pb collisions at the LHC by the ATLAS and CMS experiments using Run 2 data. Since then, heavy-ion experiments at the LHC have...

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  104. Pavle Tsotskolauri (Ivane Javakhishvili Tbilisi State University (GE))
    19/05/2026, 15:43

    he Tile Calorimeter (TileCal) is a sampling hadronic calorimeter covering the central region of the ATLAS experiment, using steel absorbers and plastic scintillators as the active medium. The High-Luminosity phase of the Large Hadron Collider (HL-LHC), expected to start operation around 2030, will deliver five times the nominal instantaneous luminosity of the LHC. To meet the resulting...

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  105. Dr Suraj Prasad (HUN-REN Wigner Research Centre for Physics (HU))
    19/05/2026, 15:45

    Heavy-ion collisions are primarily studied to investigate the properties of hot and dense primordial nuclear matter, known as the quark–gluon plasma (QGP). However, recent observations of hydrodynamic flow–like behavior in pp and p–Pb collisions at the LHC suggest the possible formation of QGP droplets even in small collision systems. To bridge the multiplicity gap between small and large...

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  106. Lucas Ferrandi (University of Münster & University of São Paulo)
    19/05/2026, 15:46

    This study identifies jets containing a J/$\psi$ meson among their constituents and defines the fragmentation function as the longitudinal momentum fraction of the jet carried by the J/$\psi$. Measuring this observable provides insights into quarkonium production mechanisms, parton-shower dynamics, and their interplay. The substantial upgrades of the ALICE detector in Run 3, most notably the...

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  107. Sweta Singh (Aligarh Muslim University (IN))
    19/05/2026, 15:47

    Event-by-event mean transverse momentum fluctuations of relativistic charged particles produced in Pb--Pb collisions at $\sqrt s_{NN} = $ 5.36 TeV are studied in terms of normalized two-particle correlator $\sqrt{C_{m}}/\langle \langle p_{T} \rangle \rangle$. Data collected using the ALICE detector during Run 3 are analyzed for this purpose and the results are compared with those reported...

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  108. Nida Malik (Aligarh Muslim University (IN))
    19/05/2026, 15:48

    Investigations involving the event-by-event fluctuations of conserved quantities, like net charge, net baryon number, and strangeness in heavy-ion collisions, provide insights into the properties of QGP and the phase diagram of strongly interacting matter. Event-by-event fluctuations of net electric charge in pp collisions at $\sqrt{s} = 13$ and $13.6$ TeV and for OO, Ne--Ne, and Pb--Pb...

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  109. Kangkan Goswami (Indian Institute of Technology Indore)
    19/05/2026, 15:49

    In non-central heavy-ion collisions, due to a non-zero impact parameter, a substantial angular momentum is produced. Through spin--orbit coupling, this angular momentum can induce quark polarization, which may subsequently manifest as a net polarization of produced hyperons and spin alignment of vector mesons. The measurement of hyperon polarization and vector meson spin alignment in pp...

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  110. Sonali Padhan (Universita di Brescia (IT))
    19/05/2026, 15:50

    In relativistic heavy-ion collisions at the LHC, extreme conditions are created where the temperature exceeds the QCD phase transition threshold ($T_{\mathrm{ch}} \sim 156$ MeV), leading to the formation of the quark--gluon plasma (QGP). In this phase, lattice QCD predicts a partial restoration of chiral symmetry, which can be investigated through parity-partner resonances with identical...

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  111. Dr Uliana Dmitrieva (Universita e INFN Torino (IT))
    19/05/2026, 15:51

    The first experimental results from the ALICE Collaboration on the emission of forward protons accompanied by neutrons in ultraperipheral $^{208}$Pb–$^{208}$Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV are presented. While electromagnetic dissociation (EMD) events with low neutron multiplicities are predominant at the LHC energies, the cross sections for the emission of one, two, and three...

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  112. Bobby McGovern (University of Victoria (CA))
    19/05/2026, 15:52

    A search is performed for the electroweak pair production of charginos and associated production of a chargino and neutralino, each of which decays through an R-parity-violating coupling into a lepton and a W, Z, or Higgs boson. This search targets the Higgs boson decay channel, using events with three or more b-tagged jets and one or two electons or muons. The analyzed dataset corresponds to...

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  113. Paula Martinez Suarez (CERN)
    19/05/2026, 15:53

    The ATLAS Level-1 trigger is a hardware-based system that selects meaningful events from the LHC, reducing the initial event rate of 40 MHz down to 100 kHz. Traditionally, Level-1 Trigger algorithms have been designed to target a set of predefined, interesting Physics signatures. However, in recent years, anomaly detection (AD) triggers have also been explored, aiming to increase the...

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  114. Sukanya Sinha (The University of Manchester (GB))
    19/05/2026, 15:54

    Trigger bandwidth limitations constrain physics analyses that target low-mass resonances, where high-rate data collection is essential. To circumvent this limitation Trigger-Level Analysis (TLA) can be applied. A recent publication by the ATLAS experiment demonstrated this approach during LHC Run 2 by processing a massive dataset of over 60 billion events, more than twice the number of fully...

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  115. Giovanni Padovano (Sapienza Universita e INFN, Roma I (IT))
    19/05/2026, 15:55

    The High-Luminosity LHC is the Large Hadron Collider long term program targeting to operate the accelerating machine at the instantaneous luminosity of 7.5 x 10^34 cm^-2 s^-1, corresponding to approximately 200 pp interactions per bunch-crossing. The ATLAS Trigger System will be upgraded to cope with such a high rate of incoming particles. The ATLAS collaboration has endorsed a upgraded...

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  116. Somanko Saha, Somanko Saha (Université Paris-Saclay (FR))
    19/05/2026, 15:56

    Precise and efficient muon detection is essential for a wide range of physics analyses at the LHC. The excellent performance of the ATLAS Muon Spectrometer (MS) during Run-1 and Run-2 enabled many key physics results, including electroweak measurements, Higgs boson studies, and searches for physics beyond the Standard Model. With the start of Run-3, the ATLAS muon system has been significantly...

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  117. Waqas Halim
    19/05/2026, 15:57

    The High-Luminosity Large Hadron Collider (HL-LHC) faces a two-pronged challenge: first, data management and analysis has become more complex and needs to be prioritized. For this purpose, the ever-evolving nature of AI warrants a shift from conventional apprenticeship-based training methods to more scalable workforce development infrastructure. At the same time, quantum-based methods, which...

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  118. Yuri do Nascimento Lima (Universidade de Sao Paulo (USP) (BR))
    19/05/2026, 15:58

    The recent injection of oxygen beams into Run 3 of the Large Hadron Collider (LHC) opens the way for the study of particle production in an unexplored energy regime. Particularly, a proton-oxygem (p-O) collision provides a favorable environment for investigating the asymmetric production of higher-density particles. This asymmetry can increase the sensitivity to the internal structure of the...

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  119. Olga Bessidskaia Bylund, Olga Bessidskaia Bylund (Université Paris-Saclay (FR))
    19/05/2026, 15:59

    In ultra-pheripheral photonuclear interactions, the colliding ions are separated by more than the sum of their radii and the reaction proceeds via photon emission from one nucleus followed by interaction with the target nucleus. A vector meson can be produced if the photon interacts with gluons in the target. Such processes are sensitive to the nuclear structure, including modifications to the...

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  120. Ms Tejaswini Thallapalli, Tejaswini Thallapally
    19/05/2026, 16:00

    Studies at the $Z$-pole have played an important role in developing our understanding of the Standard Model (SM). Continuing the explorations in this regime, we consider the possibility of the production of two $b$-quarks and a photon in proton-proton collisions at the HL-LHC. While such a final state is possible in the SM by means of the process $Z\rightarrow b\bar b$ decay with a radiated...

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  121. Marco Leitão (IPhT-Saclay & LIP-Lisbon)
    19/05/2026, 16:01

    The building block of jet quenching calculations is the differential matrix-element to radiate a gluon off a highly-energetic parton in a dense QCD medium. Analytical expressions were presented more than 30 years ago in the pioneering work of BDMPS-Z. However, exact solutions have remained elusive, thus hampering the precision of jet quenching phenomenology.

    We present the first calculation...

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  122. Manuel Kunkel
    19/05/2026, 16:02

    Composite Higgs models provide a well-motivated solution to the naturalness problem. The top quark appears as a partially composite state, generating its large mass by mixing with top partners. Besides the common vector-like quarks, also more exotic baryons can appear, including sextets of $SU(3)_c$. We present the phenomenology of such states, focusing on the expected signatures at the LHC....

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  123. Rachit Sharma (Indian Institute of Science Education and Research Thiruvananthapuram, India)
    19/05/2026, 16:03

    Leptoquarks (LQs), colour-triplet bosons that couple quarks and leptons, arise naturally in several Beyond the Standard Model (BSM) frameworks and constitute well-motivated targets for searches at the Large Hadron Collider (LHC). This work presents a comprehensive study of LQ phenomenology through refined reinterpretations of LHC Run II data and investigations of new production channels...

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  124. Dr Francesco Giovanni Celiberto (UAH Madrid)
    19/05/2026, 16:04

    Precision studies of electroweak processes at the LHC increasingly require theoretical predictions that incorporate both higher-order QCD corrections and resummation effects in the high-energy regime. In this work we present the first high-energy-resummed predictions for Drell-Yan plus jet production, providing differential spectra in rapidity and transverse momentum for $Z/\gamma^*$ bosons....

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  125. Irene Andreou (Imperial College (GB))
    19/05/2026, 16:05

    Backgrounds from quark- and gluon-initiated jets misidentified as hadronically decaying tau leptons ($\tau_\mathrm{h}$) are a major challenge in analyses involving tau leptons at CMS. Traditional methods estimate this contribution using low-dimensional parametrisations that can struggle to model complex regions of phase space. We present MUFFIN (MUltivariate Fake-Factor INference), a...

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  126. Felipe J. Llanes-Estrada
    19/05/2026, 16:06

    We deploy Quantum Chromodynamics (QCD) in Light-front Quantization (and Gauge), discretized and truncated in both Fock -- and momentum -- spaces with a particle-register encoding suited for quantum simulation; we show for the first time how to calculate fragmentation functions, a problem heretofore untractable in general from \emph{ab-initio} approaches. We provide a classical-simulator based...

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  127. Dr Duanqing Liu (Central China Normal University CCNU (CN))
    19/05/2026, 16:07

    A study of the charmless baryonic decays $B^0_{(s)} \to K^0 p \bar{p}$ is presented, where $B^0_{(s)}$ denotes either a $B^0$ or a $B^0_s$ meson. The analysis is based on proton-proton collision data collected by the LHCb experiment at centre-of-mass energies of 7, 8, and $13~\mathrm{Tev}$, corresponding to an integrated luminosity of $9~\mathrm{fb}^{-1}$. The decay $B^0_s \to K^0 p \bar{p}$...

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  128. Valerii Kholoimov (EPFL - Ecole Polytechnique Federale Lausanne (CH))
    19/05/2026, 16:08

    The COmpact DEtector for EXotics at LHCb (CODEX-b) is a particle physics detector dedicated to displaced decays of exotic long-lived particles (LLPs), compelling signatures of dark sectors Beyond the Standard Model, which arise in theories containing a hierarchy of scales and small parameters. The CODEX-b detector is a cube of high-performance RPC triplet chambers with 10 m per side, with two...

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  129. Aleksandra Petkovic (Laboratoire Leprince-Ringuet, Ecole Polytechnique)
    19/05/2026, 16:09

    Charmonium mesons are among the most important probes of deconfined QCD matter. A complete understanding of their production and interaction with the medium created in the collision is necessary to disentangle genuine hot-matter effects from cold nuclear matter effects. To achieve this, charmonium production must be measured in different collision systems over a wide energy range. Fixed-target...

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  130. Alois Caillet (Centre National de la Recherche Scientifique (FR))
    19/05/2026, 16:10

    Precise determinations of the CKM matrix element ∣Vub∣ are essential for testing the consistency of the Standard Model and for probing possible sources of flavour-changing new physics. LHCb offers a unique environment to study ∣Vub​∣ using semileptonic decays of various species of beauty hadrons, exploiting excellent vertexing, particle identification, and kinematic reconstruction. This...

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  131. Edoardo Mariani (Centre National de la Recherche Scientifique (FR), LPNHE, Sorbonne Université)
    19/05/2026, 16:11

    We present a study of the charmless three-body decays $B^0_{(s)} \to K_S^0 h^+ h^{'-}$, where $h$ is either a $\pi$ or a $K$, corresponding to 6 final states whose branching fractions are measured simultaneously. These decays are suppressed and, in certain cases, are dominated by penguin topologies. The data sample collected at LHCb between 2011 and 2018 is used for these measurements,...

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  132. Theo Cuisset (LLR / École Polytechnique (FR))
    19/05/2026, 16:12

    The High Luminosity LHC (HL-LHC) will introduce unprecedented levels of pileup, posing major challenges for particle reconstruction in dense environments. To maintain excellent physics performance, the CMS experiment will install the High Granularity Calorimeter (HGCAL), a novel endcap calorimeter system providing fine three-dimensional spatial resolution and precision timing for energy...

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  133. Youngwan Kim (Seoul National University (KR))
    19/05/2026, 16:13

    This poster presents a search for a right-handed W boson (W_R) and a heavy neutrino (N) in the Left-Right Symmetric Model, using the full CMS Run 2 dataset at 13 TeV. The analysis targets the final state with a hadronic tau, a leptonic tau, and jets from the decay chain W_R to tau N, N to tau_l jj.

    A novel strategy is employed to enhance sensitivity in both resolved and boosted regimes. For...

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  134. Dr Anuj Chandra (Aligarh Muslim University (IN))
    19/05/2026, 16:14

    One of the primary objectives of the Compressed Baryonic Matter (CBM) experiment at Facility for Antiproton and Ion Research (FAIR) is to explore the nature of QCD-phase transition at relatively high baryon density and moderate temperature, in contrast to the heavy-ion collisions at RHIC and LHC energies. In this exploration, the multifractal analysis approach can play an important role in...

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  135. Caleb Walker Fairchild (University of California Davis (US))
    19/05/2026, 16:16

    We present a search for vector-like quarks (VLQ) which decay to third-generation quarks and vector bosons in all hadronic final states. This doublet model search analyzes data from 138 fb^(−1) integrated luminosity at 13 TeV center of mass energy proton-proton collisions collected by the CMS detector. Highly Boosted jets are classified as W, Z, Higgs, top, bottom, and QCD by training a neural...

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  136. Farrah Simpson (Princeton University)
    19/05/2026, 16:17

    A search for the pair production of a vector-like quark with electric charge 5/3 (X_{5/3}), a heavy fermionic partner of the top quark, is presented. The search is performed in the single-lepton final state using proton–proton collision data collected by the CMS experiment at the LHC at a center-of-mass energy of 13 TeV during the 2016–2018 period, corresponding to an integrated luminosity of...

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  137. Ms Dorottya Cynolter, Dorottya Judit Cynolter (Eotvos Lorand University (HU))
    19/05/2026, 16:18

    Previous measurements of heavy ion collisions exhibit a suppression of high-transverse-momentum particle yield, often associated with the formation of a deconfined medium. The phenomenon has not been observed in asymmetric proton-lead collisions, motivating the study of systems of intermediate size. We present the measurement of the nuclear modification factor of charged particles in...

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  138. Licheng ZHANG (University of Maryland (US))
    19/05/2026, 16:20

    The Barrel Timing Layer (BTL) of the CMS MIP Timing Detector is entering a key integration phase at the Tracker Integration Facility (TIF). Current activities focus on the practical readiness for installation into the BTST, including rails and insertion tooling, support and roller-block elements, service integration, cabling, and tray pre-commissioning. Reception and commissioning tests on...

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  139. Mingxuan Zhang (Peking University (CN))
    19/05/2026, 16:21

    For the High Luminosity-LHC, the CMS detector is undergoing a major upgrade that includes the addition of a MIP Timing Detector (MTD). The central part of the MTD, the Barrel Timing Layer (BTL), is designed to measure the arrival time of charged particles with a precision of 30 ps. The detector units of BTL are mounted on the cooling plate to form a tray. Tray building and testing is the last...

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  140. Maria Jose (University of Virginia (US))
    19/05/2026, 16:22

    As part of the High Luminosity-LHC upgrade, a MIP Timing Detector (MTD) is being added to the CMS detector. Its central component, the Barrel Timing Layer (BTL), is designed to measure the arrival time of charged particles with a precision of 30 ps. The basic unit of the BTL is a Sensor module, created by sandwiching LYSO scintillating crystals between Silicon Photomultipliers (SiPMs)....

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  141. Gamze Sokmen (Centre National de la Recherche Scientifique (FR))
    19/05/2026, 16:23

    The High Luminosity LHC (HL-LHC) will significantly increase event rates and pileup, requiring reconstruction algorithms that remain efficient and robust in heavily populated environments. CMS will address this challenge by replacing its endcap calorimeters with the High Granularity Calorimeter (HGCAL), providing fine three dimensional position of the energy deposits and precision timing. To...

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  142. Yash Kumar (Indian Institute of Science Education and Research (IN))
    19/05/2026, 16:24

    A search for vector-like leptons that couple to standard model leptons is presented. The analysis targets vector-like lepton (doublet) models featuring two mass-degenerate states, a charged lepton (E) and a neutral lepton (N), with masses up to 1.6 TeV. The search is based on proton-proton collision data collected by the CMS experiment at the LHC, corresponding to integrated luminosities of...

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  143. Hong Gao (Beihang University (CN))
    19/05/2026, 16:25

    We present a search for the electroweak production of two Z bosons in association with two jets at a center-of-mass energy of 13 TeV. The analysis focuses on the decay channel with two charged leptons (electrons or muons) and two neutrinos, which features a relatively large branching fraction but also suffers from sizable backgrounds and incomplete event reconstruction due to the presence of...

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  144. Giovanni Celotto (University of Zurich (CH))
    19/05/2026, 16:27

    During Long Shutdown 3, the Large Hadron Collider (LHC) at CERN will undergo an upgrade program, marking the beginning of the High-Luminosity era. The High-Luminosity Large Hadron Collider (HL-LHC) is expected to collide protons at a centre-of-mass energy of 14 TeV and to reach the unprecedented peak instantaneous luminosity of 7 x 10^34 cm^-2 s^-1 with the average number of pileup events...

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  145. Huiling Hua (Chinese Academy of Sciences (CN))
    19/05/2026, 16:28

    The first study of four top quark production in final states with hadronically decaying tau leptons (th) is presented using proton-proton collision data collected by the CMS experiment at a center-of-mass energy of 13 TeV during the 2016–2018 period at the CERN LHC. This dataset corresponds to an integrated luminosity of 138 fb−1. The tau channel is divided into subchannels with zero, one, and...

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  146. Vladislav Shalaev (Joint Institute for Nuclear Research (RU))
    19/05/2026, 16:29

    A measurement of the eight angular polarization coefficients, A0 to A7, in the Drell– Yan process cross section is presented using the dimuon final state. The analysis is based on proton–proton collision data recorded with the CMS detector at the LHC at a center-of-mass energy of \sqrt(s) = 13 TeV, corresponding to an integrated luminosity of 138fb^(-1). The coefficients are determined double...

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  147. Ruben Forti (Universita & INFN Pisa (IT))
    19/05/2026, 16:30

    This poster presents the measurement of the W boson mass (mW) at the CMS experiment, published in 2024 and representing the most precise determination at the LHC, with an uncertainty of 9.9 MeV. The poster covers some of the most important aspects of the analysis, with a particular focus on the detailed measurement of the muon efficiency scale factors, which play a fundamental role in ensuring...

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  148. Elise Maria Le Boulicaut Ennis (Yale University (US))
    19/05/2026, 16:31

    The ATLAS Collaboration at CERN has developed a wide array of resources to support informal education for all ages. From colouring books and activity sheets for children, to fact sheets and cheat sheets for more advanced learners, ATLAS Outreach provides a collection of printable resources that can be used to learn more about particle physics and the ATLAS detector. In particular, ATLAS...

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  149. Dilia Maria Portillo Quintero (TRIUMF (CA))
    19/05/2026, 16:32

    Since 2010, ATLAS Virtual Visits have revolutionised HEP outreach by connecting its collaboration members with audiences worldwide. The Virtual Visit model brings inspiring scientific outreach events to visitors who would otherwise not have such an opportunity. Over the years, by offering the visits in a variety of languages and using a variety of online platforms, we have expanded their...

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  150. Giovanni Rupnik Boero (CERN / Universite de Geneve (CH))
    19/05/2026, 16:33

    The first ATLAS search for non-resonant Higgs boson pair production in association with a top-quark pair ($ttHH$) is presented. The search targets three distinct final states expected from the $ttHH$ decay: (i) one lepton (electron or muon) with at least four b-quarks, (ii) at least two b-quarks accompanied by a same-sign dilepton pair or multiple leptons, and (iii) at least three b-quarks...

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  151. Vincenzo Triglione (CPPM, Aix-Marseille Université, CNRS/IN2P3 (FR))
    19/05/2026, 16:34

    The High-Luminosity Large Hadron Collider (HL-LHC) will open new opportunities for the study of rare processes, including Higgs boson pair (di-Higgs) production. Flavour tagging will play a central role in enabling these measurements. This poster presents the expected challenges for flavour tagging in the HL-LHC environment, characterized by unprecedented instantaneous luminosity, high pile-up...

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  152. Chamathka Nirmani Thotamuna Wijewardhana (Stony Brook University (US))
    19/05/2026, 16:35

    GNTau is a hybrid graph transformer-based neural network algorithm for the identification of the visible decay products of hadronic taus, used by the ATLAS experiment in Run 3 of the LHC. The algorithm is inspired by [Nature Commun. 17 (2026) 541] and supersedes the previous recurrent neural network (RNN) based approach [ATL-PHYS-PUB-2022-044]. Information from reconstructed charged-particle...

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  153. Adam Warnerbring (Universitaet Siegen (DE))
    19/05/2026, 16:36

    We present an analysis developed to measure the CKM matrix element $|V_{cb}|$ using on-shell hadronic W boson decays in single lepton $t\bar{t}$ events collected by the ATLAS experiment at the LHC. The analysis targets Run~2 (pp) collision data at a centre-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 140 fb$^{-1}$. Existing determinations of $|V_{cb}|$ rely on...

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  154. Cen Mo (Shanghai Jiao Tong University (CN))
    19/05/2026, 16:38

    The HH → bbττ channel is among the most sensitive final states for probing Higgs boson pair production at the LHC, benefiting from the large H → bb branching fraction and the clean signatures of τ decays. The analysis is nevertheless challenged by significant backgrounds from $t\bar{t}$, Z+heavy flavour, single-Higgs production, and multijet processes. This poster presents the inclusive...

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  155. Dr Shubhalaxmi Rath (Universidad Mayor)
    19/05/2026, 16:39

    We have studied how weak momentum anisotropy, generated by the asymptotic expansion of baryon asymmetric matter in the initial stages of ultrarelativistic heavy ion collisions, modifies the charge and the heat transport coefficients and their associated observables. The electrical and the thermal conductivities are computed by solving the relativistic Boltzmann transport equation in the...

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  156. Prof. Haifa I Alrebdi (Department of Physics, College of Science, Princess Nourah bint Abdulrahman University, P.O. Box 84428, Riyadh 11671, Saudi Arabia))
    19/05/2026, 16:40

    Soft hadron production in heavy-ion collisions is sensitive to the degree of equilibration and to the strength of collective expansion, both of which vary strongly with collision centrality. We study identified-hadron transverse-momentum (pT) spectra in Pb–Pb collisions at √sNN = 2.76 TeV over centralities from 0–5% to 80–90% using a Tsallis-type parameterization to extract the effective...

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  157. Sezen Sekmen (Kyungpook National University (KR))
    19/05/2026, 17:00
  158. Simone Devoto (Universiteit Gent)
    19/05/2026, 17:30
  159. Ankita Mehta (CERN)
    19/05/2026, 18:00
  160. Ezra Lesser (Los Alamos National Laboratory)
    20/05/2026, 08:30
  161. Gherardo Vita
    20/05/2026, 09:00
  162. Marco Giacalone (CERN)
    20/05/2026, 09:30
  163. Jesse Thaler (MIT)
    20/05/2026, 10:00
  164. Romain Schotter (Austrian Academy of Sciences (AT))
    20/05/2026, 11:00
  165. Marco Colonna (Technische Universitaet Dortmund (DE))
    20/05/2026, 11:00
  166. Raoul Henderson (University of Cambridge (GB)), Raoul Henderson (Université Paris-Saclay (FR))
    20/05/2026, 11:00
  167. Benjamin Fuks
    20/05/2026, 11:00
  168. Diana Mareen Hoppe (Technische Universitaet Dresden (DE))
    20/05/2026, 11:00
  169. Yuan Zhang (University of Science and Technology of China (CN))
    20/05/2026, 11:15
  170. Martin Rybar (Charles University (CZ))
    20/05/2026, 11:18
  171. Knut Zoch (CERN)
    20/05/2026, 11:18
  172. Christos Anastopoulos (University of Sheffield (GB))
    20/05/2026, 11:18
  173. Robert Franken, Robert Franken (JMU Würzburg)
    20/05/2026, 11:18
  174. Daniele Fasanella (Universita e INFN, Bologna (IT))
    20/05/2026, 11:30
  175. Ms Dorottya Cynolter, Dorottya Judit Cynolter (Eotvos Lorand University (HU))
    20/05/2026, 11:36
  176. Otto Heinz Hindrichs (University of Rochester (US))
    20/05/2026, 11:36
  177. Irene Andreou (Imperial College (GB))
    20/05/2026, 11:36
  178. Giulia Lavizzari (Universita & INFN, Milano-Bicocca (IT))
    20/05/2026, 11:36
  179. Davide Malito (Royal Holloway, University of London (GB))
    20/05/2026, 11:45
  180. Samuel Belin (Université Paris-Saclay (FR))
    20/05/2026, 11:54
  181. Chenliang Wong (The University of Texas at Austin)
    20/05/2026, 11:54
  182. Christian Sonnabend (CERN, Heidelberg University (DE))
    20/05/2026, 11:54
  183. Sabine Wedam Lammers (Indiana University (US))
    20/05/2026, 11:54
  184. Yunfan Liu (Central China Normal University CCNU (CN))
    20/05/2026, 12:00
  185. Anke Biekoetter (KIT Karlsruhe)
    20/05/2026, 12:12
  186. Govert Hugo Nijs (CERN)
    20/05/2026, 12:12
  187. Roman Kogler (DESY (DE))
    20/05/2026, 12:12
  188. Pol Vidrier Villalba (University of Barcelona (ES))
    20/05/2026, 12:12
  189. Gemma Tinti (INFN e Laboratori Nazionali di Frascati (IT))
    20/05/2026, 12:15
  190. Simone Francescato (Harvard University (US))
    20/05/2026, 14:00
  191. Daniel Stremmer (KIT)
    20/05/2026, 14:00

    15' presentation + 3' discussion

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  192. Ella Wood (University of Cambridge (GB)), TBC
    20/05/2026, 14:00
  193. Joao Pires (LIP - Laboratorio de Instrumentação e Física Experimental de Partículas (PT))
    20/05/2026, 14:00
  194. Ken Mimasu (University of Southampton)
    20/05/2026, 14:00
  195. Laetitia Marie Guerry (Université Clermont Auvergne (FR))
    20/05/2026, 14:15
  196. Rene Poncelet (IFJ PAN Krakow)
    20/05/2026, 14:18
  197. Nikolaos Rompotis (University of Liverpool (UK))
    20/05/2026, 14:18
  198. Alessandro Broggio
    20/05/2026, 14:18

    15' presentation + 3' discussion

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  199. Giulia Marinelli
    20/05/2026, 14:22
  200. Kirill Ivanov (Massachusetts Inst. of Technology (US))
    20/05/2026, 14:30
  201. Izaac Sanderswood (Univ. of Valencia and CSIC (ES))
    20/05/2026, 14:36
  202. Rafael Coelho Lopes De Sa (University of Massachusetts (US))
    20/05/2026, 14:36
  203. Jelena Jovicevic (Institute of Physics, University of Belgrade (RS))
    20/05/2026, 14:36

    15' presentation + 3' discussion - ATLAS speaker

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  204. Andrea Bulla (Universita e INFN, Padova (IT))
    20/05/2026, 14:44
  205. Pavel Reznicek (Charles University (CZ))
    20/05/2026, 14:45
  206. Lisa Benato (Austrian Academy of Sciences (AT))
    20/05/2026, 14:54
  207. Andrea Malara (Universite Libre de Bruxelles (BE))
    20/05/2026, 14:54
  208. Jindrich Lidrych (Universite Catholique de Louvain (UCL) (BE))
    20/05/2026, 14:54

    15' presentation + 3' discussion - CMS speaker

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  209. Anni Kauniskangas (EPFL)
    20/05/2026, 15:00
  210. Alexis Vallier (L2I Toulouse, CNRS/IN2P3, UT3)
    20/05/2026, 15:06
  211. Louis Moureaux (Hamburg University (DE))
    20/05/2026, 15:12
  212. Juraj Klaric (University of Zagreb (HR))
    20/05/2026, 15:12
  213. Pierre Mayencourt (EPFL - Ecole Polytechnique Federale Lausanne (CH))
    20/05/2026, 15:15
  214. Tim Lukas
    20/05/2026, 15:30
  215. Alberto Bragagnolo (CERN)
    20/05/2026, 16:00
  216. Marzia Bordone (University of Zürich and CERN)
    20/05/2026, 16:30
  217. Renato Quagliani (CERN)
    20/05/2026, 17:00
  218. Liupan An (Peking University (CN))
    20/05/2026, 17:30
  219. Andreas Juttner (CERN)
    20/05/2026, 18:00
  220. Qipeng Hu (University of Science and Technology of China (CN))
    21/05/2026, 09:00
  221. Liliana Apolinario (LIP (PT))
    21/05/2026, 09:30
  222. Preeti Dhankher Lesser (Nikhef National institute for subatomic physics (NL))
    21/05/2026, 10:00
  223. Zhiyong Lu (China Institute of Atomic Energy (CN))
    21/05/2026, 11:00
  224. Daniel Schulte (CERN)
    21/05/2026, 11:00
  225. Theo Heimel (UCLouvain)
    21/05/2026, 11:00
  226. Rosy Caliri
    21/05/2026, 11:00
  227. Prof. Juan Terron Cuadrado (Universidad Autonoma de Madrid (ES))
    21/05/2026, 11:00
  228. Adrian Irles (IFIC CSIC/UV)
    21/05/2026, 11:18
  229. Jean-Yves OLLITRAULT
    21/05/2026, 11:18
  230. Lorenzo Valente (University of Hamburg)
    21/05/2026, 11:18
  231. Heribertus Bayu Hartanto (Asia Pacific Center for Theoretical Physics (APCTP), Pohang, South Korea)
    21/05/2026, 11:18
  232. Yanjun Tu (University of Hong Kong (HK))
    21/05/2026, 11:18
  233. Martin Spousta (Charles University)
    21/05/2026, 11:36
  234. Ayodele Ore
    21/05/2026, 11:36
  235. Roberto Preghenella (INFN, Bologna (IT))
    21/05/2026, 11:36
  236. Ilia Kalaitzidou (Universite Libre de Bruxelles (BE))
    21/05/2026, 11:36
  237. Jose Enrique Palencia Cortezon (Universidad de Oviedo (ES))
    21/05/2026, 11:36
  238. Magdalena Djordjevic
    21/05/2026, 11:54
  239. Dr Sascha Diefenbacher (Institut für Theoretische Physik, Universität Heidelberg)
    21/05/2026, 11:54
  240. Carlos Moreno Martinez (Universite de Geneve (CH))
    21/05/2026, 11:54
  241. Enzo Canonero (Royal Holloway, University of London (GB))
    21/05/2026, 11:54
  242. Armin Ilg (University of Zurich)
    21/05/2026, 11:54
  243. Thorsten Wengler (CERN)
    21/05/2026, 12:12
  244. Biao Zhang (Heidelberg university(DE))
    21/05/2026, 12:12
  245. Jiuzhao Li (Central China Normal University CCNU (CN))
    21/05/2026, 12:12
  246. Dawei Fu (Peking University (CN))
    21/05/2026, 12:12
  247. David Rohr (CERN)
    21/05/2026, 12:12
  248. Iwona Grabowska-Bold (AGH University of Krakow (PL))
    21/05/2026, 14:00
  249. Daina Leyva Pernia (Deutsches Elektronen-Synchrotron (DE))
    21/05/2026, 14:00
  250. Luca Buonocore (CERN)
    21/05/2026, 14:00
  251. Dr Arunima Bhattacharya (Instituto de Física Corpuscular (University of Valencia), Spain)
    21/05/2026, 14:00

    15' presentation + 3' discussion

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  252. Christiane Scherb
    21/05/2026, 14:00
  253. Mr Stefan Kluth (Max Planck Society (DE))
    21/05/2026, 14:18
  254. Miguel Fernandez Gomez (Universidade de Santiago de Compostela (ES))
    21/05/2026, 14:18
  255. Katrin Greve
    21/05/2026, 14:18
  256. Noemi Palmeri (Sapienza Universita e INFN, Roma I (IT))
    21/05/2026, 14:18
  257. Simone Tentori (UCLouvain)
    21/05/2026, 14:18

    15' presentation + 3' discussion

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  258. Qiuchan Lu (LLR, Centre National de la Recherche Scientifique (FR))
    21/05/2026, 14:36
  259. Danijela Bogavac (IFAE)
    21/05/2026, 14:36

    15' presentation + 3' discussion - ATLAS speaker

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  260. Farouk Mokhtar (Univ. of California San Diego (US))
    21/05/2026, 14:36
  261. John Stupak (University of Oklahoma (US))
    21/05/2026, 14:36
  262. Tommaso Saracco (Nikhef)
    21/05/2026, 14:36
  263. Manal Alsairafi
    21/05/2026, 14:54

    In this talk I present NLO QCD predictions for the $$pp\to t\bar{t}t\bar{t}+X$$ process in the 4 lepton decay channel at the integrated and differential level for the LHC centre-of-mass energy of $$\sqrt{s}=13.6$$ TeV. Specifically I compare the fixed order NLO QCD calculations to the parton-shower matched results obtained with MC@NLO and POWHEG matching. In the former, NLO QCD corrections...

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  264. Mathis Frahm (Hamburg University (DE))
    21/05/2026, 14:54

    15' presentation + 3' discussion - CMS speaker

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  265. Oscar Garcia-Montero (Universität Bielefeld)
    21/05/2026, 14:54
  266. Francisco Sili (University of Science and Technology of China (CN))
    21/05/2026, 14:54
  267. Matthias Kleiner (CERN)
    21/05/2026, 14:54
  268. Ana Sculac (University of Split. Fac.of Elect. Eng., Mech. Eng. and Nav.Architect. (HR))
    21/05/2026, 15:12

    Focus on full Run 2 data, with HL-LHC projections - CMS speaker (15' presentation + 3' discussion)

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  269. Dukhishyam Mallick (Universita e INFN, Cagliari (IT))
    21/05/2026, 15:12
  270. Jiahui Zhuo (Univ. of Valencia and CSIC (ES))
    21/05/2026, 15:12
  271. Huiling Hua (Chinese Academy of Sciences (CN))
    21/05/2026, 15:12
  272. Romain Bouquet (INFN - University of Genova (Italy))
    21/05/2026, 15:12
  273. Eleni Vryonidou (University of Cyprus (CY))
    21/05/2026, 16:00
  274. Marina Kolosova (University of Florida (US))
    21/05/2026, 16:30
  275. Alessandro Tarabini (ETH Zurich (CH))
    21/05/2026, 17:00
  276. Dr Kei Yagyu (Osaka University)
    21/05/2026, 17:30
  277. Diallo Boye (Brookhaven National Laboratory)
    21/05/2026, 18:00
  278. Nazar Burmasov (Joint Institute for Nuclear Research (RU))
    22/05/2026, 09:00
  279. Giovanni Limatola
    22/05/2026, 09:30
  280. Nedaa Alexandra Asbah (CERN), Nedaa Alexandra Asbah (CERN)
    22/05/2026, 10:00
  281. Christopher Mc Ginn (Massachusetts Inst. of Technology (US))
    22/05/2026, 11:00
  282. Thomas Flacke (KIAS)
    22/05/2026, 11:00
  283. Nicolo Lai (Universita e INFN, Padova (IT))
    22/05/2026, 11:00

    15' presentation + 3' discussion - CMS speaker

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  284. Mark Smith (Imperial College (GB))
    22/05/2026, 11:00
  285. Konstantin Schmid (University and INFN Padova)
    22/05/2026, 11:00

    15' presentation + 3' discussion

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  286. Valerii Kholoimov (EPFL - Ecole Polytechnique Federale Lausanne (CH))
    22/05/2026, 11:18
  287. Betsy Cunnett (University of Sussex (GB))
    22/05/2026, 11:18

    15' presentation + 3' discussion

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  288. Samantha Abbott (University of California Davis (US))
    22/05/2026, 11:18
  289. Egor Antipov (Stony Brook University (US))
    22/05/2026, 11:18

    Including BSM decays, invisible BR constraint, exclusive decays - ATLAS speaker (15' presentation + 3' discussion)

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  290. Carlota Andres (CPHT, Ecole polytechnique)
    22/05/2026, 11:18
  291. Weronika Stanek-Maslouska (Deutsches Elektronen-Synchrotron (DE))
    22/05/2026, 11:36
  292. Ajdin Palavric (IFIC Valencia)
    22/05/2026, 11:36

    15' presentation + 3' discussion

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  293. Yvonne Ng (Univ. Illinois at Urbana Champaign (US))
    22/05/2026, 11:36
  294. Judita Mamužić (Jožef Štefan Institute (SI))
    22/05/2026, 11:36
  295. Lisa Biermann
    22/05/2026, 11:36

    15' presentation + 3' discussion

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  296. Alfredo Glioti (INFN - Roma)
    22/05/2026, 11:54

    15' presentation + 3' discussion

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  297. Carlos Javier Barbero Pretel (Universidade de Santiago de Compostela (ES))
    22/05/2026, 11:54
  298. Luc Tomas Le Pottier (University of California Berkeley (US))
    22/05/2026, 11:54

    15' presentation + 3' discussion - ATLAS speaker

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  299. Gael Coulon (Centre National de la Recherche Scientifique (FR))
    22/05/2026, 11:54
  300. Anton Stepennov (University of Cyprus (CY))
    22/05/2026, 11:54
  301. Giacomo Boldrini (CERN)
    22/05/2026, 12:12

    15' presentation + 3' discussion

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  302. Jingyu Zhang (Vanderbilt University (US))
    22/05/2026, 12:12
  303. Matthias Steinhauser (KIT)
    22/05/2026, 12:12

    15' presentation + 3' discussion

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  304. Dr Christian Appelt (Tel Aviv University (IL))
    22/05/2026, 12:12
  305. Malgorzata Kazana (NCBJ Warsaw (PL))
    22/05/2026, 12:12
  306. Luc DARME
    22/05/2026, 14:00
  307. Roberta Cardinale (INFN e Universita Genova (IT))
    22/05/2026, 14:00
  308. Michele Selvaggi (CERN)
    22/05/2026, 14:00
  309. Kateryna Radchenko Serdula (DESY)
    22/05/2026, 14:00
  310. Rebeca Beltrán (University of Cyprus)
    22/05/2026, 14:00
  311. Lorenzo Paolucci (The University of Manchester (GB))
    22/05/2026, 14:18
  312. Matthew Forslund (Princeton Center for Theoretical Science)
    22/05/2026, 14:18
  313. Andrea Pizarro Medina
    22/05/2026, 14:18
  314. 22/05/2026, 14:18
  315. Meng Lu (Northeastern University (US))
    22/05/2026, 14:18
  316. Matteo Defranchis (CERN)
    22/05/2026, 14:36
  317. Pruthvi Suryadevara (Tata Institute of Fundamental Research (IN))
    22/05/2026, 14:36
  318. Tong Qiu (The University of Edinburgh (GB))
    22/05/2026, 14:36
  319. Ivaylo Dionisov (Sofia University St. Kliment Ohridski (BG))
    22/05/2026, 14:36
  320. Michael Hoch (KIT - Karlsruhe Institute of Technology (DE))
    22/05/2026, 14:36
  321. Dr Yang Ma (UCLouvain)
    22/05/2026, 14:54
  322. Carlos Escobar Ibañez (Instituto de Física Corpuscular (IFIC), CSIC‐UV, Spain)
    22/05/2026, 14:54
  323. Elise Maria Le Boulicaut Ennis (Yale University (US))
    22/05/2026, 14:54
  324. Jihun Kim (Seoul National University), Jihun Kim (Seoul National University), Jihun Kim (Seoul National University (KR))
    22/05/2026, 14:54
  325. Pallabi Das (CERN)
    22/05/2026, 14:54
  326. 22/05/2026, 15:12
  327. Margaret Lutz (University of Toronto (CA))
    22/05/2026, 15:12
  328. Luis Pascual Dominguez (Universidad Autonoma de Madrid (ES))
    22/05/2026, 15:12
  329. Giacomo Da Molin (Laboratory of Instrumentation and Experimental Particle Physics (PT))
    22/05/2026, 15:12
  330. Dr Yang-Ting Chien (Georgia State University)
    22/05/2026, 15:12
  331. 22/05/2026, 16:00
  332. Viola Sordini (Centre National de la Recherche Scientifique (FR))
    22/05/2026, 16:10
  333. Chiara Mariotti (INFN Torino (IT))
    22/05/2026, 16:40
  334. Michelangelo Mangano (CERN)
    22/05/2026, 17:10
  335. Sarah Marie Demers (Yale University (US))
    22/05/2026, 17:40
  336. Guy Wilkinson (University of Oxford (GB))
    22/05/2026, 17:50
  337. Francesco Sannino (University of South Denmark (DK))