20–24 Apr 2026
CERN
Europe/Zurich timezone

Contribution List

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  1. Yoav Afik (University of Chicago (US))
    20/04/2026, 13:00
  2. Nicolas Brunner (University of Geneva)
    20/04/2026, 13:15
  3. Beatrix Hiesmayr (IT:U Austria)
    20/04/2026, 14:00
  4. Massimo Blasone (Università di Salerno and INFN)
    20/04/2026, 14:25
  5. Michael Doser (CERN)
    20/04/2026, 14:50
  6. David Kaiser (MIT)
    20/04/2026, 16:00

    The hundredth anniversary of quantum mechanics in 2025-26 offers opportunities to consider the history of quantum theory and ask how some of our core ideas were introduced, debated, tested, and ultimately accepted. One of the most central conceptual ingredients of quantum theory is entanglement, nowadays so important to the burgeoning field of quantum information science and technology. Yet...

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  7. Alberto Navarro (Seoultech)
    21/04/2026, 09:00
  8. Giovanni Pelliccioli (Università degli Studi di Milano-Bicocca)
    21/04/2026, 09:25
  9. Tairan Xu (University of Michigan (US))
    21/04/2026, 09:50
  10. Jeffrey Davis (Johns Hopkins University (US))
    21/04/2026, 10:15
  11. Dong Woo Kang (JBNU)
    21/04/2026, 11:10
  12. Otto Heinz Hindrichs (University of Rochester (US))
    21/04/2026, 11:35
  13. Fiona Ann Jolly (Deutsches Elektronen-Synchrotron (DE))
    21/04/2026, 12:00
  14. Kamila Kowalska (National Centre for Nuclear Research)
    21/04/2026, 14:00
  15. Carlos Wagner
    21/04/2026, 14:25
  16. Ian Low
    21/04/2026, 14:50
  17. Spencer Chang (University of Oregon)
    21/04/2026, 15:45
  18. Navin McGinnis
    21/04/2026, 16:10
  19. Nikos Mavromatos (University of London (GB))
    21/04/2026, 16:35
  20. Arthur Wu
    22/04/2026, 09:00
  21. Sagar Hazra
    22/04/2026, 09:25
  22. Antonio Di Domenico (Sapienza Universita e INFN, Roma I (IT))
    22/04/2026, 09:50
  23. Emidio Gabrielli (Nat. Inst. of Chem.Phys. & Biophys. (EE))
    22/04/2026, 10:15
  24. Claude Duhr
    22/04/2026, 11:10
  25. Juan Antonio Aguilar Saavedra (Consejo Superior de Investigaciones Científicas (ES))
    22/04/2026, 11:35
  26. Fabio Cerutti (Lawrence Berkeley National Lab. (US))
    22/04/2026, 12:00
  27. Rafael Aoude
    22/04/2026, 14:00
  28. Liantao Wang
    22/04/2026, 14:25
  29. Marcel Vos (IFIC Valencia (ES))
    22/04/2026, 14:50
  30. Joonwoo Bae (Korea Advanced Institute of Science and Technology)
    22/04/2026, 15:45
  31. Albert Rico
    22/04/2026, 16:10
  32. Vlatko Vedral
    22/04/2026, 16:35
  33. Beatrix Hiesmayr (IT:U Austria), Regina Demina (University of Rochester (US))
    22/04/2026, 17:20
  34. Enrico Speranza (CERN)
    23/04/2026, 09:15
  35. Zhoudunming Tu
    23/04/2026, 09:40
  36. Thomas Richardson (UC Berkeley)
    23/04/2026, 10:05
  37. Rebecca von Kuk (Univerisity of Bern)
    23/04/2026, 11:00
  38. Dmitri Kharzeev
    23/04/2026, 11:25
  39. Chris White (Queen Mary University of London)
    23/04/2026, 14:00
  40. Giorgio Busoni (Adelaide University)
    23/04/2026, 14:25
  41. Zhewei Yin
    23/04/2026, 14:50
  42. Alba Cervera Lierta (Barcelona Supercomputing Center)
    23/04/2026, 16:00
  43. Kazuki Sakurai (University of Warsaw)
    23/04/2026, 16:25
  44. Pawel Horodecki (Gdansk University of Technology)
    23/04/2026, 17:00

    Quantum mechanics is a very special physical theory where randomness is built in on the ontological level. In particular it allows quantum correlations – also called quantum entanglement – that are stronger than all the correlations we know from our daily lives.
    Einstein's ingenious skepticism about this theory gave rise to the fundamental philosophical question - formalized...

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  45. Prof. Christopher Timpson (University of Oxford), Juan Ramon Munoz De Nova
    23/04/2026, 18:00
  46. Kun Cheng (University of Pittsburgh)
    24/04/2026, 09:15
  47. Yoshitaka Hatta (BNL)
    24/04/2026, 09:40
  48. Tao Han
    24/04/2026, 10:05
  49. Andreas Werner Jung (Purdue University (US))
    24/04/2026, 11:00
  50. Alan Barr (University of Oxford (GB))
    24/04/2026, 11:25
  51. Radoslaw Piotr Grabarczyk (University of Oxford (GB))

    We prove that measurements of decay directions of unstable particles can in principle rule out any local hidden variable model in which the response function is analytic i.e. has a convergent power series expansion at each point on the sphere. Ruling out such a large class of theories can in practice be approached by ruling out local hidden variable models with sequentially less...

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  52. Olimpia Miniati

    Within the framework currently adopted for the description of the fundamental interactions, the particles involved in high-energy collisions are expected to exhibit a basic quantum behaviour.
    As a consequence of this statement, a novel class of "quantum" observables for collider studies naturally arises, whose physical interpretation is rooted in the characteristics of the underlying quantum...

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  53. Dr Danilo Micali Fucci (Faculty of Philosophy, University of Oxford)

    Collider proposals for Bell tests with unstable particles (e.g., $H \to ZZ^{\ast},\; WW^{\ast}$) face two structural issues: measurement settings are not freely choosable, and the boson-pair spin density matrix is inferred indirectly from decay kinematics through QFT-based reconstruction, obscuring the operational meaning of the Bell observables and introducing theory dependence in the...

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  54. Prof. Fabio Maltoni (Universite Catholique de Louvain (UCL) (BE) and Università di Bologna)

    The Quantum Observables approach to High Energy Physics is an emerging framework in which observables borrowed from Quantum Information theory are used to test the Standard Model and explore BSM Physics. This methodology received experimental validation in 2023-2024, when the ATLAS and CMS collaborations reported measurements, via quantum tomography, of entanglement in $t\bar{t}$ pairs...

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  55. Ivo Young (University of Glasgow (GB))

    Reconstructing dileptonic $t\bar{t}$ events remains a long-standing challenge due to the presence of two undetectable neutrinos. Many techniques still in use today have seen little change over the past three decades. This poster gives an overview of the reconstruction algorithms currently used by the ATLAS experiment: Neutrino Weighting, Sonneschein and Ellipse Method, and a novel...

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  56. Ms ROJALIN PADHAN (CAU, Seoul)

    We investigate entanglement generation in Higgs scattering processes within SMEFT, treating the weak isospin as qubit. For 2→2 Higgs scattering, we calculate the von Neumann entropy to measure entanglement between the momentum and isospin degrees of freedom in the final state, and concurrence to quantify two-qubit entanglement within the isospin subspace. We examine whether these entanglement...

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  57. Alan Herrera (University of Rochester (US))

    Recent LHC measurements enable the study of the quantum state of top quark-antiquark ($t\bar{t}$) pairs via the spin degree of freedom. Using the CMS measurement of $t\bar{t}$ spin correlations in the helicity and beam bases, we evaluate a set of quantum information observables, including discord, steerability, Bell correlation, and magic. These observables provide a quantitative...

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  58. Guillermo García Mir (Univ. of Valencia and CSIC (ES))

    In this contribution we explore the potential of colliders - existing facilities like Belle II and the LHC and the future Higgs/top/EW factory - to study interacting quantum systems. We present projections for the statistical significance of the decoherence due to final-state radiation in top quark pair production at the LHC and at an e+e- collider and in tau-lepton pair production in...

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  59. Sung Won Yun (KAIST)

    Entanglement corresponds to quantum correlations that have no classical counterparts. Its detection can be realized by estimation of a collection of observables that constitute entanglement witnesses (EWs), for which, however, no systematic method of their construction is known so far. In this work, we introduce a supermap-based framework for detecting entanglement generation in quantum...

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  60. Ondrej Penc (Czech Academy of Sciences (CZ))

    Quantum discord quantifies non-classical correlations beyond entanglement and is defined as the difference between two quantum generalizations of mutual information constructed from von Neumann entropies. For top-antitop pairs, the discord can be estimated analytically under the Bell-diagonal approximation, where it becomes a function of the spin-correlation coefficients and can be directly...

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  61. 지헌 성 (Korea Advanced Institute of Science and Technology)

    Entanglement witnesses (EWs) provide a powerful and flexible method for detecting entanglement in quantum systems. Recently, mirrored entanglement witnesses have been introduced, revealing that a single EW can admit nontrivial upper bounds and thus be paired with a mirrored witness [1]. This framework significantly enhances the detection capability of EWs by allowing entanglement to be...

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  62. Thomas Driscoll (University of Oregon)

    We study how virtual next-to-leading-order (NLO) electroweak corrections affect quantum-information resources in lepton-lepton collisions. Interpreting helicity amplitudes as multi-qudit quantum states, we quantify entanglement and magic in the processes $\ell^+\ell^- \to \tau^+\tau^-,\, WW,\, ZZ$. Including one-loop corrections, we construct the corrected helicity density matrices and...

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  63. Avalon Roberts (The University of Manchester (GB))

    New sources of CP violation beyond those described in the Standard Model are required to explain the observed matter–antimatter asymmetry of the Universe. The Standard Model Effective Field Theory provides a framework to introduce additional electroweak sources of CP-odd physics in a model-independent manner. Suppressed in polarisation-blind observables, traditional probes of these New Physics...

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  64. Masanori Tanaka

    In this talk, we discuss the entanglement entropy produced by decaying particles and its implications for the parameters in the Standard Model (SM). The decay out-states of unstable particles provide a unique, well-defined intrinsic quantum-information probe of the SM parameter space. We focus on Higgs decays as an example in this presentation. After tracing out kinematics, we compute...

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  65. Laurel Carpenter (University of Rochester (US))

    Following recent LHC measurements of entanglement in top quark-antiquark pairs ($t\bar{t}$), the next step towards a deeper understanding of quantum correlations is to investigate whether this entanglement persists when one of the pair decays into a $W$ boson and a bottom (anti-)quark. The $tW$ system, formed by the $W$ boson and the remaining top quark, provides the unique opportunity to...

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  66. Angelo Arisi (Purdue University (US))

    The measurement of quantum observables at colliders is fundamental not only as a test of quantum mechanics properties at high energies but also for their sensitivity to BSM effects.
    Top quark has been found to be an ideal candidate to study these properties in high energy physics, as demonstrated by the recent measurement of entanglement in top pair production at LHC. In particular, a final...

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  67. Dong Woo Kang (Jeonbuk National University)

    The two-photon collision option of a linear e+e− collider, a photon linear collider, is using the back-scattered laser photons off the incident electrons and positrons. The polarizations of the colliding photons can be controlled by using the polarized initial electrons and positrons and the polarized laser beams. We study the impact of the polarizations of the colliding photons on observation...

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  68. Mr Enzo Ghilardi Nogueira (Max-Planck-Institut für Physik), Mr Felipe Recio Busquier (Max-Planck-Institut für Physik)

    B°/anti-B° pairs produced in the decays of the Upsilon(4S) and (5S) are supposed to be in an entangled state. At the (4S) it should be antisymmetric C=-1 state, at the (5S) both the antisymmetric (C=-1) and the symmetric (C=+1) state are possible.
    The entanglement at the (4S) is an important condition for the measurement of time dependent CP violation, any admixture of other states would...

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  69. Mira Varma (Yale University (US))

    The Born rule is a central postulate of quantum mechanics and underlies all probabilistic predictions in collider physics, yet direct experimental tests of this assumption have largely been confined to low-energy systems. In this work, we investigate how spin and polarization measurements at high-energy colliders can probe the Born rule at TeV energies. Focusing on experimentally accessible...

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