Contribution List

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  1. Prof. Ki-jeong LEE (Hanyang University)
    22/09/2025, 09:30
  2. Prof. Jin Hee Yoon (Inha University (KR))
    22/09/2025, 09:40
  3. Su Yong Choi (Korea University (KR))
    22/09/2025, 09:50
  4. Tae Jeong Kim (Hanyang University (KR))
    22/09/2025, 10:05
  5. Juan Antonio Aguilar Saavedra (Consejo Superior de Investigaciones Científicas (ES))
    22/09/2025, 10:15
  6. Nadezhda Proklova (University of Pennsylvania (US))
    22/09/2025, 11:30
  7. Markus Seidel (Riga Technical University (LV))
    22/09/2025, 12:00
  8. Tomas Dado (CERN)
    22/09/2025, 12:30
  9. Heribertus Bayu Hartanto (Asia Pacific Center for Theoretical Physics (APCTP), Pohang, South Korea)
    22/09/2025, 14:30
  10. Sebastian Wuchterl (CERN)
    22/09/2025, 15:00
  11. Johannes Hessler (Max Planck Society (DE))
    22/09/2025, 15:30
  12. Leon Mans (RWTH Aachen University)
    22/09/2025, 16:00
  13. Sergio Sanchez Cruz (CERN)
    22/09/2025, 17:00
  14. Stergios Kazakos (Michigan State University (US))
    22/09/2025, 17:30
  15. Judith Katzy (Deutsches Elektronen-Synchrotron (DE))
    22/09/2025, 18:00
  16. Javier Del Riego Badas (Universidad de Oviedo (ES))
    22/09/2025, 18:30
  17. Jiwon Park (Deutsches Elektronen-Synchrotron (DE))
    22/09/2025, 19:30
  18. Yeonsu Ryou (Hanyang University (KR))
    22/09/2025, 19:35
  19. Ivo Young (University of Glasgow (GB))
    22/09/2025, 19:40
  20. Lukas Kretschmann (Bergische Universitaet Wuppertal (DE))
    22/09/2025, 19:45
  21. Raees Ahmad Khan (University of Pittsburgh (US))
    22/09/2025, 19:50
  22. Ya-Juan Zheng
    22/09/2025, 19:55
  23. Dhimiter Canko (Università di Bologna)
    22/09/2025, 20:00
  24. Colomba Brancaccio (University of Turin)
    22/09/2025, 20:05
  25. Mr Souvik Bera
    22/09/2025, 20:10
  26. JINHEUNG KIM
    22/09/2025, 20:15
  27. Aman Desai (Adelaide University (AU))
    22/09/2025, 20:20
  28. Louise Beriet
    22/09/2025, 20:25
  29. Dr Long Chen (Shandong University)
    23/09/2025, 09:30
  30. Fiona Ann Jolly (Deutsches Elektronen-Synchrotron (DE))
    23/09/2025, 10:00
  31. Nils Faltermann (KIT - Karlsruhe Institute of Technology (DE))
    23/09/2025, 10:30
  32. Mr Changqiao Li (Max Planck Society (DE))
    23/09/2025, 11:30
  33. Ian Moult
    23/09/2025, 12:00
  34. Marco Zaro (Università degli Studi e INFN Milano (IT))
    23/09/2025, 14:00
    EFT
  35. Mr Marcos Miralles Lopez (University of Glasgow)
    23/09/2025, 14:30
    EFT
  36. Andrea Piccinelli (University of Notre Dame (US))
    23/09/2025, 15:00
    EFT
  37. Maheyer Jamshed Shroff (University of Victoria (CA))
    23/09/2025, 15:30
    EFT
  38. 23/09/2025, 16:00
  39. Hao-lin Li (Zhongshan University), Dr Haolin Li (CP3/UCLouvain)
    23/09/2025, 16:40
  40. Jiwon Park (Deutsches Elektronen-Synchrotron (DE))
    23/09/2025, 17:10
  41. Gilberto Tetlalmatzi-Xolocotzi (Siegen University)
    23/09/2025, 17:40
  42. Normunds Ralfs Strautnieks (University of Latvia (LV))
    23/09/2025, 18:10
  43. Maarten De Coen (Ghent University (BE))
    24/09/2025, 09:30
  44. Katharina Voss (Universitaet Siegen (DE))
    24/09/2025, 09:45
  45. Christian Biello (Max-Planck Institute for Physics)
    24/09/2025, 10:00
  46. Gino Daniels (Purdue University (US))
    24/09/2025, 10:15
  47. Huacheng Cai (CERN)
    24/09/2025, 10:30
  48. Van Dung Le (Vietnam National University (VN))
    24/09/2025, 10:45
  49. Min Tang (ZJU - Zhejiang University (CN))
    24/09/2025, 11:00
  50. Maren Stratmann (Bergische Universitaet Wuppertal (DE))
    24/09/2025, 11:15
  51. Hesham El Faham (The University of Manchester)
    24/09/2025, 12:00
  52. Diptaparna Biswas (Universitaet Siegen (DE))
    24/09/2025, 12:30
  53. Kaoru Hagiwara (KEK)
    25/09/2025, 09:30
  54. Yuichiro Kiyo (Tohoku University)
    25/09/2025, 10:00
  55. Giovanni Limatola
    25/09/2025, 10:30
  56. Benjamin Fuks
    25/09/2025, 11:30
  57. Prof. Jeonghyeon Song (Konkuk University)
    25/09/2025, 12:00
  58. Romal Kumar
    25/09/2025, 12:30
  59. Didar Dobur (Ghent University (BE))
    25/09/2025, 13:00
  60. Reza Goldouzian (University of Notre Dame (US))
    25/09/2025, 14:30
  61. Oliver Majersky (Deutsches Elektronen-Synchrotron (DE))
    25/09/2025, 15:00
  62. Anna Kulesza (University of Muenster)
    25/09/2025, 15:30
  63. Jan van der Linden (Ghent University (BE))
    25/09/2025, 16:00
  64. Josh McFayden (University of Sussex)
    25/09/2025, 17:00
  65. Maryam Shooshtari (Austrian Academy of Sciences (AT))
    25/09/2025, 17:30
  66. Dominic Hirschbuehl (Bergische Universitaet Wuppertal (DE))
    25/09/2025, 18:00
  67. Andre Govinda Stahl (CERN)
    25/09/2025, 18:30
  68. 25/09/2025, 22:30
  69. Pawel Horodecki (Gdansk University of Technology)
    26/09/2025, 09:30
  70. Matteo Defranchis (CERN)
    26/09/2025, 10:00
  71. Giulia Zanderighi (Max Planck Society (DE))
    26/09/2025, 11:20
  72. Wolfgang Wagner (Bergische Universitaet Wuppertal (DE))
    26/09/2025, 12:05
  73. Tae Jeong Kim (Hanyang University (KR))
    26/09/2025, 12:50
  74. Maryam Shooshtari (Austrian Academy of Sciences (AT))
  75. Monica Verducci (Universita & INFN Pisa (IT))
    Talk

    Complex statistical tools are required for the extraction and interpretation of measurements at the LHC experiments. Tools used by ATLAS and CMS are now public, e.g. Combine and TRExFitter. These can be used for more complex actions such as multi-analysis combinations, unfolding and EFT interpretations. This talk will discuss the underlying statistical methods, including recent developments...

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  76. Jose Enrique Palencia Cortezon (Universidad de Oviedo (ES))

    A reinterpretation of four top quark (tttt) production is presented using the full Run 2 dataset recorded by the CMS experiment, corresponding to an integrated luminosity of 138/fb. The analysis targets BSM scenarios using the existing tttt production measurement, including constraints on effective field theory (EFT) operators, top-philic heavy resonances, and the top-Yukawa coupling. The...

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  77. Jose Enrique Palencia Cortezon (Universidad de Oviedo (ES))
    Poster

    A search for charged lepton flavor violation (CLFV) in top quark interactions is presented. The search uses proton-proton collision data collected with the CMS experiment at the LHC during Run2, corresponding to an integrated luminosity of 138 fb^{-1} at a center-of-mass energy of 13 TeV. The study targets both single top production via CLFV interaction and top quark pair production followed...

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  78. Monica Verducci (Universita & INFN Pisa (IT))
    Talk

    The LHC produces a vast sample of top quark pairs and single top quarks. Measurements of the inclusive top quark production rates at the LHC have reached a precision of several percent and test advanced Next-to-Next-to-Leading Order predictions in QCD. Differential measurements in several observables are important to test SM predictions and improve Monte Carlo generator predictions. In this...

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  79. Jose Enrique Palencia Cortezon (Universidad de Oviedo (ES))

    Effective Field Theory (EFT) provides a universal framework for probing beyond the Standard Model physics at LHC scales. Recent advances in analysis techniques and increased dataset complexity have significantly enhanced the sensitivity of EFT studies. We present the latest results on EFT obtained using ttbar production by the CMS collaboration, probing interactions between the top quark and...

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  80. Min Tang (ZJU - Zhejiang University (CN))
  81. Monica Verducci (Universita & INFN Pisa (IT))
    Talk

    Many-parameter fits to precise measurements in the framework of the Standard Model Effective Field Theory are becoming a standard interpretation of LHC and other collider data. In this contribution an overview is given of state-of-the-art EFT interpretations in ATLAS with particular emphasis on results in the top quark sector.

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  82. Monica Verducci (Universita & INFN Pisa (IT))
    Talk

    Many-parameter fits to precise measurements in the framework of the Standard Model Effective Field Theory are becoming a standard interpretation of LHC and other collider data. In this contribution an overview is given of state-of-the-art EFT interpretations in ATLAS with particular emphasis on results in the top quark sector.

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  83. Sofia Palacios Schweitzer (ITP, University Heidelberg)
  84. Monica Verducci (Universita & INFN Pisa (IT))
    Talk

    The exceptionally large dataset collected by the ATLAS and CMS detectors at the highest proton-proton collision energies provided by the LHC enables precision testing of theoretical predictions using an extensive sample of top quark events. One example of this is the spin correlation of top quarks, which can uniquely be probed due to the decay time being shorter than hadronisation time. This...

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  85. Jose Enrique Palencia Cortezon (Universidad de Oviedo (ES))
    Poster

    A violation of the charge-parity (CP) symmetry can explain the paradox of the baryon asymmetry of the universe. We have studied a forward-backward asymmetry of an angular distribution defined in the top quark sector, which is strongly related to the CP-violation. The measurement is performed in the t-channel production of single top quark in proton-proton collisions, at center-of-mass energy...

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  86. Byeonghak Ko (Sejong University (KR))
  87. Monica Verducci (Universita & INFN Pisa (IT))
    Talk

    The exceptionally large dataset collected by the ATLAS and CMS detectors at the highest proton-proton collision energies provided by the LHC enables precision testing of theoretical predictions using an extensive sample of top quark events. One example of this is the spin correlation of top quarks, which can uniquely be probed due to the decay time being shorter than hadronisation time. This...

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  88. Dr Souvik Bera (Asia Pacific Center for Theoretical Physics)
    Poster

    We present analytic expressions for the one-loop QCD helicity amplitudes contributing to top-quark pair production in association with a photon or a jet at the Large Hadron Collider (LHC), evaluated through $O(\epsilon^2)$ in the dimensional regularisation parameter, $\epsilon$. These amplitudes are required to construct the two-loop hard functions that enter the NNLO QCD computation. The...

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  89. Prof. Seong Chan Park (Yonsei University)
  90. Roberto Tenchini (Universita & INFN Pisa (IT))
  91. Mr Syed Haider Ali (Department of Physics & Applied Mathematics, Pakistan Institute of Engineering and Applied Sciences (PIEAS), P. O. Nilore 45650, Islamabad)

    Rare event classification in high-energy physics (HEP) plays a crucial role in probing physics beyond the Standard Model (BSM). Such processes serve as indirect searches for new physics by testing deviations from SM predictions in extreme kinematic regimes. The production of four top quarks in association with a ($W^-$) boson at $(\sqrt{s} = 13)$ $ TeV$ is an exceptionally rare SM process with...

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  92. Syed Haider Ali
  93. Van Dung Le (Vietnam National University (VN))

    We will report on an extensive survey of rare and exclusive few-body decays of the top quark, defined as those with branching fractions BR≲$10^{-5}$ and two or three final-state particles [1]. Such rare decays probe physics beyond the Standard Model (BSM), constitute a background for exotic decays into new BSM particles, and provide precise information on quantum chromodynamics factorization...

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  94. Monica Verducci (Universita & INFN Pisa (IT))
    Talk

    The high center-of-mass energy of proton-proton collisions and the large available datasets at the CERN Large Hadron Collider allow the study of rare processes of the Standard Model with unprecedented precision. Measurements of rare SM processes provide new tests of the SM predictions with the potential to unveil discrepancies with the SM predictions or provide important input for the...

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  95. Monica Verducci (Universita & INFN Pisa (IT))
    Talk

    The top-quark mass is one of the key fundamental parameters of the Standard Model that must be determined experimentally. Its value has an important effect on many precision measurements and tests of the Standard Model. The Tevatron and LHC experiments have developed an extensive program to determine the top quark mass using a variety of methods. In this contribution, the top quark mass...

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  96. Aman Desai (University of Adelaide (AU))
    Poster

    Recent results from the CMS experiment at the Large Hadron Collider indicate the presence of a top-quark pair bound state near the $t\bar{t}$ threshold region. We present a way to reconstruct a toponium state at the ttbar threshold region formed at the Large Hadron Collider using Recursive Jigsaw Reconstruction. We have considered the Non-Relativistic QCD based toponium model implemented in...

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  97. Monica Verducci (Universita & INFN Pisa (IT))
    Talk

    This talk is to present new techniques in ATLAS for object reconstruction and identification

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  98. Jose Enrique Palencia Cortezon (Universidad de Oviedo (ES))

    A search for the standard model Higgs boson decaying to a cc pair, produced in association with a tt pair (ttH) is presented. The search is performed with the full Run 2 dataset, corresponding to an integrated luminosity of 138/fb. Advanced machine learning techniques are employed for jet flavor identification and event classification. The H->bb decay is measured simultaneously. The...

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  99. Doğa Elitez (CERN)
    Poster

    We present the first search for Higgs boson pair production in association with top quarks ($t\bar{t}HH$), using proton–proton collision data recorded by the ATLAS detector, corresponding to the full Run 2 and partial Run 3 datasets. The $t\bar{t}HH$ process is the third most significant production mode for Higgs boson pairs at the LHC and offers direct sensitivity to the anomalous...

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  100. Prof. Jose Enrique Palencia Cortezon (Universidad de Oviedo (ES))
    Poster

    We present studies of the b_bbar_4l (bb4l) package from the POWHEG BOX RES Monte Carlo generator, used to model top quark productions for the CMS experiment at the LHC. The bb4l package includes next-to-leading order matrix element calculations interfaced to parton shower for top quark pair production, the associated production of a single top quark with a W boson, their interferences, and the...

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  101. Ya-Juan Zheng
    Poster

    We study the single top plus Higgs production process at the LHC with a CP violating Yukawa coupling from a dimension-6 operator. The amplitude of the subprocess ub>dtH is obtained both in the Unitary (U) and Feynman-Diagram (FD) gauges. Energy and angular distributions of the cross section and CP violating asymmetries are understood from the interference among the FD gauge amplitudes.

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  102. JINHEUNG KIM
    Poster

    Many Beyond the Standard Model (BSM) theories predict new scalar bosons 𝜙 that couple to top quarks. Such scalars contribute to $gg\to t\bar{t}$ production via $gg\to \phi^* \to t\bar{t}$, leading to significant interference with the Standard Model $gg\to t\bar{t}$ amplitude. Near the $t\bar{t}$ threshold, top quark pairs form bound states, requiring careful theoretical treatment of the...

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  103. Prof. Jian Wang (Shandong University)
    Poster

    We present the first analytic results of next-to-next-to-next-to-leading-order (N3LO) QCD corrections to the top-quark decay width. We focus on the dominant leading color contribution, which includes light-quark loops. At next-to-next-to-leading order (NNLO), this dominant contribution accounts for 95% of the total correction. By utilizing the optical theorem, the N3LO corrections are related...

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  104. Prof. Jian Wang (Shandong University)
  105. Monica Verducci (Universita & INFN Pisa (IT))
    Talk

    The high center-of-mass energy of proton-proton collisions and the large available datasets at the CERN Large Hadron Collider allow the study of rare processes of the Standard Model with unprecedented precision. Measurements of rare SM processes provide new tests of the SM predictions with the potential to unveil discrepancies with the SM predictions or provide important input for the...

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  106. Markus Klute (Karlsruhe Inst. of Technology (GER))
    Poster

    The Future Circular Collider (FCC) programme provides unique opportunities for comprehensive and precise studies of top quark physics. At the FCC-ee, operating at and slightly above the top pair threshold, a precise measurement of the top quark mass with a statistical and systematic accuracy down to the MeV level can be achieved through a threshold scan. Furthermore, the FCC-ee run at 365 GeV...

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  107. Chiara Signorile

    In this presentation, we will discuss recent advancements in NNLO+PS predictions for top-quark pair production and decay within the MiNNLO framework. MiNNLO provides a robust method for incorporating next-to-next-to-leading order (NNLO) QCD corrections directly into fully differential predictions, offering unprecedented accuracy. This approach enables a consistent treatment of both production...

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  108. Chiara Signorile
  109. Christian Biello (Max-Planck Institute for Physics)

    The current MiNNLOPS technology enables next-to-next-to-leading order (NNLO) QCD predictions matched to parton showers (NNLO+PS) for heavy-quark pair production in arbitrary kinematics (QQF), within the POWHEG framework. Among QQF processes, Higgs production in association with a heavy-quark pair is particularly relevant for LHC phenomenology. In the case of ttH production, the main bottleneck...

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  110. Dhimiter Canko (Università di Bologna)
    Poster

    We present the calculation of two-loop Feynman integrals contributing to NNLO QCD corrections to the production of a top-quark pair in association with a W boson at hadron colliders, in the leading colour approximation. This process constitutes a key signature at the Large Hadron Collider, and the precise prediction of its cross-section is imperative for comparisons with experimental data. In...

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  111. Colomba Brancaccio
    Poster

    I will present the calculation of two-loop QCD amplitudes for the radiative top decay process t->Wbg, with the W-boson decay to a lepton-neutrino pair included. This amplitude is required in the computation of top quark pair production in association with a jet at NNLO QCD accuracy where the top decays are included in the narrow width approximation. Analytic form of the two-loop helicity...

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