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Christophe Royon (The University of Kansas (US)), Fotios Ptochos (University of Cyprus (CY)), Dr Georgios Krintiras (The University of Kansas (US))04/09/2023, 09:00
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Amanda Sarkar (University of Oxford (GB))04/09/2023, 09:10
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Achim Geiser (Deutsches Elektronen-Synchrotron (DE))04/09/2023, 09:40
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Dr Tanjona R. Rabemananjara (NIKHEF & VU Amsterdam), Tanjona Radonirina Rabemananjara (CERN)04/09/2023, 10:10
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Andreas van Hameren04/09/2023, 11:10
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Yair Mulian04/09/2023, 11:40
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Amanda Sarkar (University of Oxford (GB)), Dr Tanjona R. Rabemananjara (NIKHEF & VU Amsterdam)04/09/2023, 12:10
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Christophe Royon (The University of Kansas (US))04/09/2023, 14:00
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Istvan Szanyi (Eötvös University, Wigner RCP, MATE KRC), Mr István Szanyi (Eötvös Loránd University)04/09/2023, 14:30
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Ferenc Siklér (Wigner RCP, Budapest (HU))04/09/2023, 15:30
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Clara Elisabeth Leitgeb (Deutsches Elektronen-Synchrotron (DE))04/09/2023, 16:00
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Antoni Szczurek04/09/2023, 16:30
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Sanjin Benić04/09/2023, 17:00
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Christophe Royon (The University of Kansas (US)), Ferenc Siklér (Wigner RCP, Budapest (HU))04/09/2023, 17:30
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Edmond Iancu (Université Paris-Saclay (FR))05/09/2023, 09:00
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Tomasz Stebel (CERN), Tomasz Stebel (Institute of Theoretical Physics Jagiellonian University)05/09/2023, 09:30
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Renaud BOUSSARIE (CPHT, CNRS, Ecole polytechnique, IP Paris)05/09/2023, 10:00
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Federico Deganutti05/09/2023, 11:00
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Dionysios Triantafyllopoulos (ECT*/FBK)05/09/2023, 11:30
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Dionysios Triantafyllopoulos (ECT*/FBK), Edmond Iancu (Université Paris-Saclay (FR)), Renaud BOUSSARIE (CPHT, CNRS, Ecole polytechnique, IP Paris)05/09/2023, 12:00
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Andrea Bellora (Universita e INFN Torino (IT))05/09/2023, 14:00
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Adrien Auriol (University of Birmingham (GB))05/09/2023, 14:30
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Valery Khoze (University of Durham (GB))05/09/2023, 15:30
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Michael Pitt (The University of Kansas (US))05/09/2023, 16:00
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Amanda Sarkar (University of Oxford (GB))05/09/2023, 16:30
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Antoni Szczurek, Leszek Motyka, Michael Pitt (The University of Kansas (US))05/09/2023, 17:00
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Dr Georgios Krintiras (The University of Kansas (US))06/09/2023, 09:00
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Luis Alcerro Alcerro (The University of Kansas (US))06/09/2023, 09:30
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Antoni Szczurek06/09/2023, 10:00
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Javier Alberto Murillo Quijada (Universidad de Sonora (MX))06/09/2023, 11:00
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Jaswant Singh (Indian Institute of Technology New Delhi)06/09/2023, 11:30
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Dr Georgios Krintiras (The University of Kansas (US)), Javier Alberto Murillo Quijada (Universidad de Sonora (MX))06/09/2023, 12:00
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Achim Geiser (Deutsches Elektronen-Synchrotron (DE))07/09/2023, 09:00
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Michael Pitt (The University of Kansas (US))07/09/2023, 09:30
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Federico Deganutti07/09/2023, 10:00
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Prof. Bernd Surrow (Temple University)07/09/2023, 11:00
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Christophe Royon (The University of Kansas (US))07/09/2023, 11:30
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Achim Geiser (Deutsches Elektronen-Synchrotron (DE)), Armando Bermudez Martinez (CERN), Jean-Philippe Lansberg (Université Paris-Saclay (FR))07/09/2023, 12:00
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Prof. Bernd Surrow (Temple University)07/09/2023, 14:00
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Mr Arjun Kumar (Indian Institute of Technology Delhi)07/09/2023, 14:30
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Dr Tanjona R. Rabemananjara (NIKHEF & VU Amsterdam), Tanjona Radonirina Rabemananjara (CERN)07/09/2023, 15:30
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Emmet Byrne07/09/2023, 16:00
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Renaud BOUSSARIE (CPHT, CNRS, Ecole polytechnique, IP Paris)07/09/2023, 16:30
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Jean-Philippe Lansberg (Ecole Polytechnique), Jean-Philippe Lansberg (Ecole polytechnique), Jean-Philippe Lansberg (Université Paris-Saclay (FR))08/09/2023, 09:00
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Dr Maxim Nefedov (IJClab, Orsay)08/09/2023, 09:30
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Leszek Motyka08/09/2023, 10:00
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Prof. Bernd Surrow (Temple University)08/09/2023, 11:00
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Armando Bermudez Martinez (CERN)08/09/2023, 11:30
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Achim Geiser (Deutsches Elektronen-Synchrotron (DE)), Armando Bermudez Martinez (CERN), Jean-Philippe Lansberg (Université Paris-Saclay (FR))08/09/2023, 12:00
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Melike Akbiyik (Johannes Gutenberg Universitaet Mainz (DE))08/09/2023, 14:00
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Andrei Poblaguev (Brookhaven National Laboratory)08/09/2023, 14:30
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Marco Santimaria (INFN e Laboratori Nazionali di Frascati (IT))08/09/2023, 15:30
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Yair Mulian08/09/2023, 16:00
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Sorina Popescu (F), Sorina Popescu (The University of Kansas (US))08/09/2023, 16:30
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Achim Geiser (Deutsches Elektronen-Synchrotron (DE)), Armando Bermudez Martinez (CERN), Jean-Philippe Lansberg (Université Paris-Saclay (FR))08/09/2023, 17:00
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Christophe Royon (The University of Kansas (US)), Fotios Ptochos (University of Cyprus (CY)), Dr Georgios Krintiras (The University of Kansas (US))08/09/2023, 17:30
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Michael Pitt (The University of Kansas (US))
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Tomasz Stebel (Institute of Theoretical Physics Jagiellonian University)
We present our recent calculation of the dijet electroproduction cross section at the NLO accuracy within the Color Glass Condensate effective field theory. We focus on kinematical regime where the two jets are forward w.r.t. projectile's longitudinal direction and are almost back-to-back in transverse plain. We discuss the interplay between small-x and Sudakov resummation and show numerical...
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Dr Maxim Nefedov (IJClab, Orsay)
The formalism of gauge-invariant EFT for Multi-Regge processes in QCD is used to compute impact-factors relevant for processes of production of heavy quarkonia within Non-Relativistic QCD Factorisation formalism and High-Energy Factorisation at one-loop accuracy. The examples of $\gamma+R\to c\bar{c}\left[{}^1S_0^{[8]}\right]$ and $g+R\to c\bar{c}\left[{}^1S_0^{[1]}\right]$ impact factors will...
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Melike Akbiyik (Johannes Gutenberg Universitaet Mainz (DE))
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Jaswant Singh (Indian Institute of Technology New Delhi)
We use Machine Learning with the event-generator (Sar$t$re) for
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the for exclusive diffraction processes in electron-nucleus scattering. The second moment of the amplitude includes averaging of hundreds of initial nucleon configurations of the heavy nucleus, a procedure which is extremely CPU intense. We show that we can make the production of the cross-sections used for event generation at... -
Emmet Byrne
There has been much recent progress towards extending the BFKL equation to next-to-next-to-leading logarithmic (NNLL) accuracy. In this talk I will briefly review the status of this programme of research. I will then discuss our recent progress in extracting some of the missing ingredients of the NNLL kernel, including the one-loop central-emission vertex (CEV) for two gluons which are not...
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Arjun Kumar (Indian Institute of Technology Delhi)
This analysis provides new fits of the GBW model and the impact parameter-dependent saturation model (bSat or IP-Sat) to the leading neutron structure function HERA data in one-pion exchange approximation. Both parametrizations of the dipole cross section provide good descriptions of the considered data. It is shown here for the first time that the experimental leading neutron production HERA...
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ATLAS Collaboration
Measurements of hadron production provide important insight about the quark and gluon fragmentation that are relevant for the simulation of kinematic distributions of high-energy collisions. The measurement of charged particle distributions using LHC proton-proton data collected at 13.6 TeV of centre-of-mass energy will be presented. The differences in the production with and without...
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Sanjin Benić
In this contribution I would like to report on our recent findings [1] regarding the exclusive eta_c production in e+p and e+A collisions that is sensitive to the Odderon. We are working within the framework of Color Glass Condensate applicable at the high energies that would be reached at future electron ion colliders. The Odderon distribution at small-x is found by explicitly solving the...
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ATLAS Collaboration
The production of jets and prompt isolated photons at hadron colliders provides stringent tests of perturbative QCD. The most recent measurements in this area by the ATLAS experiment, using proton-proton collision data at $\sqrt{s}$ =13 TeV, are presented. Prompt inclusive photon production is measured for two distinct photon isolation cones, R=0.2 and 0.4, as well as for their ratio. The...
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Istvan Szanyi (Eötvös University, Wigner RCP, MATE KRC)
It is known that the Real Extended Bialas-Bzdak (ReBB) model describes the proton-proton ($pp$) and proton-antiproton ($p\bar p$) differential cross section data in a statistically not excludible way, i.e., with a confidence level greater than 0.1% in the center of mass energy range 546 GeV $\leq\sqrt{s}\leq 8$ TeV and in the squared four-momentum transfer range 0.37 GeV$^2$ $\leq -t\leq1.2$...
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Katarzyna Wichmann (Deutsches Elektronen-Synchrotron (DE))
A new measurement of inclusive jet cross sections in neutral current deep inelastic scattering using the ZEUS detector at the HERA collider is presented. The data were taken at HERA in the years 2004 to 2007 at a centre-of-mass energy of 318 GeV and correspond to an integrated luminosity of 347 pb-1. Massless jets, reconstructed using the kT-algorithm in the Breit reference frame, have been...
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Katarzyna Wichmann (Deutsches Elektronen-Synchrotron (DE))
The azimuthal decorrelation angle ∆φ between the leading jet and scattered lepton in deep inelastic scattering has been measured with the ZEUS detector at HERA.The experimental data set was taken in the HERA II data-taking period and corresponds to an integrated luminosity of 326 pb-1. The measurement was performed within a range of the exchanged photon virtuality Q2 from 10 to 350 GeV2, the...
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Prof. Bernd Surrow (Temple University)
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Yair Mulian
Using the CGC effective theory together with the hybrid factorisation, we study forward photon+jet production in proton-nucleus collisions beyond leading order. We first compute the "real" next-to-leading order (NLO) corrections, i.e. the radiative corrections associated with a three-parton final state, out of which only two are being measured. Then we move to the "virtual" NLO corrections to...
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Leszek Motyka
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Yair Mulian
For almost a century, the general solution for the Schrödinger equation was assumed to be generated by a time-ordered exponential known as the Dyson series. We discuss under which conditions the unitarity of this solution is broken, and additional discrete dynamics emerges. Then, we provide an alternative construction that is manifestly unitary, regardless of the Hamiltonian and the setup. The...
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Michael Pitt (The University of Kansas (US))
The talk will cover several research opportunities with tagged forward protons/neutrons using the proton-proton and proton-Oxygen collisions at the Large Hadron Collider.
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ATLAS Collaboration
The indirect determination of the W-boson mass from global electroweak fits outperforms the precision of its experimentally measured value. An improved experimental measurement is therefore one of the goals of the LHC physics program. The talk will present a re-analysis of the mass of the W boson at a centre-of-mass energy of 7 TeV using a profile likelihood fit, which improves the precision...
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ATLAS Collaboration
Precision measurements of the production cross-sections of Z bosons at LHC provide important tests of perturbative QCD and constrain the parton distribution functions for quarks within the proton. This talk will present an extraordinarily precise double-differential measurement of the Z boson in the full phase space of the decay leptons at a centre-of-mass energy of 8 TeV. The recoil of the...
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Jean-Philippe Lansberg (Université Paris-Saclay (FR))
I will review the impact of QCD corrections to quarkonium production in inclusive and exclusive reactions. First, I will explain how they significantly alter the cross section at mid and large $p_T$ in inclusive photo- and hadro-production. Second, I will discuss the perturbative instability arising at high energies in $p_T$-integrated fixed-order computations and discuss how they can be...
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Jean-Philippe Lansberg (IPN Orsay, Paris Saclay U. / IN2P3-CNRS), Jean-Philippe Lansberg (Ecole polytechnique), Jean-Philippe Lansberg (Université Paris-Saclay (FR))
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Katarzyna Wichmann (Deutsches Elektronen-Synchrotron (DE))
Lorentz and CPT symmetry in the quark sector of the Standard Model are studied in the context of an effective field theory using ZEUS e±p data. Symmetry-violating effects can lead to time-dependent oscillations of otherwise time-independent observables, including scattering cross sections. An analysis using five years of inclusive neutral-current deep inelastic scattering events corresponding...
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Carlos Ricardo Contreras Correa (Departamento de Fisica-Univ. Tecnica Federico Santa Maria (UTFS)
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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 polarized fixed-target collisions, by exploring a unique kinematic regime given by the LHC beam and by exploiting new probes.
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This ambitious task poses its basis on the recent installation of SMOG2, the unpolarized gas target in front of the LHCb... -
Andrei Poblaguev (Brookhaven National Laboratory)
The Polarized Hydrogen Gas Jet Target Polarimeter (HJET) at the Relativistic Heavy-Ion Collider (RHIC) is utilized to accurately measure the vertical polarization of proton beams with low systematic uncertainties of approximately $\sigma^\text{syst}_P/P\le0.5\%$. These measurements are conducted in the CNI region, $0.0013<|t|<0.017~\rm{GeV}^2$. By measuring the elastic single $A_\text{N}(t)$...
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