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Christophe Royon (The University of Kansas (US)), Sanjin Benić08/09/2025, 09:00
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Amanda Sarkar (University of Oxford (GB)), amanda sarkar08/09/2025, 09:10
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Swagato Mukherjee08/09/2025, 09:40
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Javier Jiménez-López (University of Alcalá)08/09/2025, 10:10
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Pawel Nadel-Turonski (University of South Carolina)08/09/2025, 11:10
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Daniel Savoiu (KIT), Daniel Savoiu (Hamburg University (DE))08/09/2025, 11:40
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Amanda Sarkar (University of Oxford (GB)), Daniel Savoiu (Hamburg University (DE)), Pawel Nadel-Turonski (University of South Carolina)08/09/2025, 12:10
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Agustin Sabio Vera, Prof. Agustin Sabio Vera, Mr Dario Vaccaro (Laboratório de Instrumentação e Física Experimental de Partículas (LIP))08/09/2025, 15:00
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Swagato Mukherjee08/09/2025, 15:30
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Mariusz Sadzikowski (Jagiellonian University), Mariusz Sadzikowski08/09/2025, 16:00
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Amanda Sarkar (University of Oxford (GB)), amanda sarkar08/09/2025, 17:00
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Leszek Motyka, Mariusz Sadzikowski (Jagiellonian University), Mariusz Sadzikowski08/09/2025, 17:30
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Luis Alcerro Alcerro (The University of Kansas (US))09/09/2025, 09:00
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Weronika Stanek-Maslouska (Deutsches Elektronen-Synchrotron (DE))09/09/2025, 09:30
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Christophe Royon (The University of Kansas (US))09/09/2025, 10:00
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Joseph Yarwick (IJC Lab, University Paris-Saclay)09/09/2025, 11:00
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Prof. ALESSANDRO PAPA (Università della Calabria & INFN-Cosenza), Alessandro Papa, Alessandro Papa09/09/2025, 11:30
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Christophe Royon (The University of Kansas (US)), Cyrille Marquet (CPHT - Ecole Polytechnique), Swagato Mukherjee09/09/2025, 12:00
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Frigyes Janos Nemes (CERN (also at Wigner RCP Budapest, Hungary)), Frigyes Nemes (MTA KFKI)09/09/2025, 15:00
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Tamas Csorgo (MATE Institute of Technology Karoly Robert Campus (HU)), Tamás Ferenc Csörgö (Wigner RCP Budapest and MATE Institute of Technology, Gyöngyös, Hungary)09/09/2025, 15:30
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Michael Pitt (CERN)09/09/2025, 16:00
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Mr Eric Andreas Vivoda (Department of Physics, Faculty of Science, University of Zagreb), Mr Eric Andreas Vivoda (PMF Zagreb)09/09/2025, 17:00
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Michael Pitt (CERN), Sanjin Benić09/09/2025, 17:30
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Tamas Csorgo (MATE Institute of Technology Karoly Robert Campus (HU)), Tamás Ferenc Csörgö (Wigner RCP Budapest and MATE Institute of Technology, Gyöngyös, Hungary)09/09/2025, 18:15
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Ada Solano (Universita' di Torino e INFN (IT)), Marta Ruspa (Universita e INFN Torino (IT))09/09/2025, 18:30
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Valery Khoze (University of Durham (GB))10/09/2025, 09:00
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Istvan Szanyi (MATE KRC, University of Kansas, Wigner RCP), Mr István Szanyi (Eötvös Loránd University)10/09/2025, 09:30
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Maciej Trzebinski (Polish Academy of Sciences (PL))10/09/2025, 10:00
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Andrei Poblaguev, Andrei Poblaguev (Brookhaven National Laboratory)10/09/2025, 11:00
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Krista Lizbeth Smith (Pusan National University (KR)), Krista Smith10/09/2025, 11:30
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Maciej Trzebinski (Polish Academy of Sciences (PL)), Valery Khoze (University of Durham (GB))10/09/2025, 12:00
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Bernd Surrow, Prof. Bernd Surrow (Temple University), Bernd Surrow10/09/2025, 15:00
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Jian-Ping Chen10/09/2025, 15:30
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Barbara Badelek (University of Warsaw (PL))10/09/2025, 16:00
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Kresimir Kumericki, Krešimir Kumerički10/09/2025, 17:00
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Marco Santimaria, Marco Santimaria (INFN e Laboratori Nazionali di Frascati (IT))10/09/2025, 17:30
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Barbara Badelek (University of Warsaw (PL)), Jian-Ping Chen, Marco Santimaria, Marco Santimaria (INFN e Laboratori Nazionali di Frascati (IT))10/09/2025, 18:00
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Christophe Royon (The University of Kansas (US))10/09/2025, 18:45
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Nico Timothy Toikka (Helsinki Institute of Physics (FI))11/09/2025, 09:00
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Mr Max Vanden Bemden (Universite Libre de Bruxelles (BE))11/09/2025, 09:30
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Vieri Candelise (Universita di Roma I "La Sapienza"-Universita & INFN, Roma I), Vieri Candelise (Universita e INFN Trieste (IT))11/09/2025, 10:00
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Evelin Meoni (Universita della Calabria e INFN (IT))11/09/2025, 11:00
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Keila Moral Figueroa (CMS)11/09/2025, 11:30
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Kornelija Passek-K. (Ruđer Bošković Institute, Zagreb, Croatia), Kornelija Passek-Kumerički11/09/2025, 12:00
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Evelin Meoni (Universita della Calabria e INFN (IT)), Vieri Candelise (Universita di Roma I "La Sapienza"-Universita & INFN, Roma I), Vieri Candelise (Universita e INFN Trieste (IT))11/09/2025, 12:30
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11/09/2025, 15:30
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Tetiana Hryn'ova (Centre National de la Recherche Scientifique (FR))12/09/2025, 09:00
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Javier Alberto Murillo Quijada (Universidad de Sonora (MX))12/09/2025, 09:30
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Dr Georgios Krintiras (The University of Kansas (US))12/09/2025, 10:00
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José Garrido12/09/2025, 11:00
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Ishita Ganguli12/09/2025, 11:30
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Jing Wang, Jing Wang (Massachusetts Inst. of Technology (US)), jing wang12/09/2025, 12:00
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12/09/2025, 12:30
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Sergio Javier Arbiol Val (Polish Academy of Sciences (PL))12/09/2025, 15:00
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Marcin Kucharczyk (Syracuse), Marcin Kucharczyk (Polish Academy of Sciences (PL)), Marcin Kucharczyk (Polish Academy of Sciences (PL))12/09/2025, 15:30
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Goran Duplancic (Institute Ruder Boskovic, Zagreb), Goran Duplančić12/09/2025, 16:00
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Evelin Meoni (Universita della Calabria e INFN (IT)), Vieri Candelise (Universita di Roma I "La Sapienza"-Universita & INFN, Roma I), Vieri Candelise (Universita e INFN Trieste (IT))12/09/2025, 17:00
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Christophe Royon (The University of Kansas (US)), Dr Georgios Krintiras (The University of Kansas (US)), Sanjin Benić12/09/2025, 17:45
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Mats Kampshoff (The University of Kansas)
We compute the $q\bar{q}g$ part of the NLO diffractive structure functions for deep-inelastic scattering using quasi Monte Carlo methods and compare to LO results.
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Keila Moral Figueroa (CMS)
Heavy boson densities are determined by solving extended DGLAP-type evolution equations that include all known strongly and weakly interacting partons and bosons. We use the Parton-Branching (PB) approach, which also allows for the direct extraction of Transverse Momentum Dependent (TMD) densities.
The initial distributions are fitted to high-precision Deep Inelastic Scattering data from...
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Ayman A. Al-Bataineh (Yarmouk University), Ayman Ahmad Al-Bataineh, Ayman Ahmad Al-Bataineh (U), Ayman Ahmad Al-Bataineh (University of Kansas (US))
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Swagato Mukherjee
Transverse-momentum-dependent parton distributions (TMDs) are essential for unraveling the three-dimensional structure of hadrons, forming a core scientific component of the Electron-Ion Collider (EIC) program. Employing a novel Coulomb-gauge-fixed lattice QCD approach at physical quark masses, we reliably access transverse separations up to approximately 1 fm, corresponding to the small...
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Javier Jiménez-López (University of Alcalá)
We explore the potential for the extraction of the longitudinal structure function $F_L$ and the determination of the gluon unpolarized PDF from it. The impact of differing assumptions on sample sizes, systematic uncertainties and beam energy scenarios are investigated. With a sufficiently large number of center-of-mass energy configurations and well-controlled systematics, the EIC will...
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Ishita Ganguli
We study photon-hadron Transverse Energy-Energy Correlators (TEEC) and azimuthal correlation in the forward rapidity region for pp and p$Pb$ collisions, in light of the planned detector upgrades at high luminosity LHC. The computation is based on the hybrid $k_T$ factorization, implemented at parton level in KaTie, supplemented by initial and final state radiation as well as hadronization via...
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Dr Gian Michele Innocenti (Massachusetts Inst. of Technology (US))
Ultraperipheral heavy-ion collisions (UPCs) offer a clean way to study photon–nucleus interactions at high energy. In this talk, we present the first next-to-leading order predictions for inclusive $D^0$ production in Pb–Pb UPCs at the LHC, obtained with the new G$\gamma$A–FONLL framework. The framework relies on FONLL (Fixed-Order Next-to-Leading Logarithm) to model heavy-quark production in...
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Mariusz Sadzikowski
We discuss a twist decomposition of the proton structure functions within
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the frameworks of the Balitsky-Fadin-Kurayev-Lipatov and Balitsky-Kovchegov equations and argue that in both cases the higher twist effects are strongly suppressed. This implies that unitarization effects of high energy scattering amplitudes are mostly the leading twist effect. -
Marija Rapseviciute (Vilnius University (LT))
This overview of the Monte Carlo (MC) simulation process at the four main experiments - ATLAS, CMS, ALICE, and LHCb - at the Large Hadron Collider (LHC) is provided in this talk. Given the complexity and noise of proton-proton collisions, simulated samples are essential for understanding and interpreting the experimental results, enabling precise measurements and searches for new physics. The...
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Achim Geiser (Deutsches Elektronen-Synchrotron (DE))
Fragmentation of charm and beauty quarks into charm and beauty hadrons in pp collisions at LHC has recently been measured to be nonuniversal, with deviations from universality as established from e+e- collisions by up to an order of magnitude.
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We review these measurements and find a simple entirely data-driven phenomenological parametrization of this nonuniversality. We apply this to the... -
Andrei Poblaguev
The analysis of transverse analyzing powers $A_\text{N}^{pA}(t)$ in proton-nucleus scattering, as measured by the RHIC hydrogen gas jet target polarimeter (HJET), requires precise Coulomb corrections to both spin-flip and non-flip amplitudes. These corrections must account for a broad range of nuclear charges $Z$ and form factor slopes, while allowing flexibility to vary form factors during...
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Maciej Trzebinski (Polish Academy of Sciences (PL))
A key focus of the physics program at the LHC is the study of head-on proton-proton collisions. However, an important class of physics can be studied for cases where the protons narrowly miss one another and remain intact. In such cases, the electromagnetic fields surrounding the protons can interact producing high-energy photon-photon collisions. Alternatively, interactions mediated by the...
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Leszek Motyka, Leszek Motyka
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Cyrille Marquet (CPHT - Ecole Polytechnique), Cyrille Michel Marquet (Universidade de Santiago de Compostela (ES))
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Marco Santimaria (INFN e Laboratori Nazionali di Frascati (IT))
The goal of LHCspin is to develop, in the next few years, innovative solutions and cutting-edge technologies to access spin physics in high-energy and high-intensity collisions of the LHC beam against a polarized fixed target.
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This ambitious task poses its basis on the recent success of SMOG2, the unpolarized gas target installed in front of the LHCb spectrometer. SMOG2, already itself a... -
Marcin Kucharczyk (Polish Academy of Sciences (PL))
The new results on three-pion Bose-Einstein correlations measured with the sample of proton-proton collisions recorded at the centre-of-mass energy of √s = 7 TeV will be presented, being the first study of three-particle Bose-Einstein correlations measured in the forward region provided by the LHCb detector. The results are interpreted within the core-halo model for the first time in...
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Brian Andrew Cole (Columbia University (US))
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