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Victor Mokeev (Thomas Jefferson National Accelerator Facility)9/7/26, 9:00 AM
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Daniel Carman (Jefferson Laboratory)9/7/26, 9:30 AM
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Dr Toru Sato9/7/26, 10:00 AM
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Prof. Craig Roberts9/7/26, 10:30 AM
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Dr Hiroyuki Sako (Japan Atomic Energy Agency)9/7/26, 11:30 AM
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Colin Morningstar (Carnegie Mellon University)9/7/26, 12:00 PM
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Jia-jun Wu9/7/26, 12:30 PM
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Dr Zhao Qian Yao9/7/26, 3:00 PM
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Eulogio Oset9/7/26, 3:00 PM
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Ralf Gothe9/7/26, 3:00 PM
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Daniele Binosi9/7/26, 5:30 PM
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Alessandro Pilloni (University of Messina & INFN Catania)9/7/26, 5:30 PM
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Andrea Signori (University of Turin and INFN)9/7/26, 5:30 PM
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Karin Schönning9/8/26, 9:00 AM
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Dr Reinhard Beck9/8/26, 9:30 AM
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Jean-Marc Richard (University of Lyon & CNRS-IN2P3, France)9/8/26, 10:00 AM
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Dr Maxim Mai (University of Bern)9/8/26, 10:30 AM
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Peter Hurck (University of Bonn)9/8/26, 11:30 AM
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Jung-Keun Ahn9/8/26, 12:00 PM
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Qian Wang (South China Normal University, Guangzhou, China)9/8/26, 12:30 PM
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Joannis Papavassiliou9/8/26, 3:00 PM
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Juan M Nieves9/8/26, 3:00 PM
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Kyungseon Joo (University of Connecticut)9/8/26, 3:00 PM
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Michael Doering (The George Washington University)9/8/26, 5:30 PM
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Elena Santopinto (INFN)9/8/26, 5:30 PM
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Alexey Vladimirov (Universidad Complutense de Madrid)9/8/26, 5:30 PM
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Gernot Eichmann9/9/26, 9:00 AM
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Prof. Annalisa D'Angelo (University of Roma Tor Vergata & INFN Roma Tor Vergata)9/9/26, 9:00 AM
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Raul Gonzalez Jimenez (Universidad de Sevilla)9/9/26, 9:00 AM
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Prof. Tanja Horn (Catholic University of America)9/10/26, 9:00 AM
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Dr Stefan Diehl (Justus Liebig University Giessen and University of Connecticut)9/10/26, 9:30 AM
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Prof. Marc Vaderhaeghen9/10/26, 10:00 AM
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Dr Juan M. Cruz Martinez (Universidad de Sevilla)9/10/26, 10:30 AM
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Dr Oleg Denisov (INFN, sezione di Torino)9/10/26, 11:30 AM
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Prof. Feng Kun Guo9/10/26, 12:00 PM
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Dr Sergey Syritsin9/10/26, 12:30 PM
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John Bulava9/10/26, 3:00 PM
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Chandan Mondal9/10/26, 3:00 PM
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Achim Gerold Denig (JGU Mainz)9/10/26, 3:00 PM
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Sara Collins9/10/26, 5:30 PM
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Jose Manuel Alarcón (Universidad de Alcalá)9/10/26, 5:30 PM
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Cédric Mezrag9/10/26, 5:30 PM
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Jacqueline Keintzel (CERN)9/11/26, 9:00 AM
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Frank Nerling (GSI Darmstadt & GU Frankfurt)9/11/26, 9:30 AM
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Marc Illa (PNNL)9/11/26, 10:00 AM
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Noemi Rocco (IFIC - Universitat de Valencia)9/11/26, 10:30 AM
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Prof. Jacquelyn Noronha-Hostler (University of Illinois Urbana Champaign)9/11/26, 11:30 AM
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William King Brooks Jr (Federico Santa Maria Technical University (CL))9/11/26, 12:00 PM
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Evgeny Epelbaum (Ruhr-University Bochum)9/11/26, 12:30 PM
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Frank Nerling (GSI Darmstadt & GU Frankfurt)
A newly established initiative has successfully been launched to strengthen the First Science (+) programme of the upcoming FAIR accelerator facility, also in view of anti-protons delivered by the High Energy Storage Ring in the future. While investigating fundamental questions related to the strong interaction in the non-perturbative regime, employing high-intensity proton and secondary pion...
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Deborah Rönchen
The Jülich-Bonn model is a well-established dynamical coupled-channel approach that has been applied in recent years primarily to study the spectrum of light baryon resonances from pion- and photon-induced reactions with different hadronic final states. In this talk, I will present the adaptation of the framework to kaon-induced reactions with the goal to extract the spectrum of resonances...
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Sara Collins
Through the calculation of nucleon matrix elements both in
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the forward and off-forward kinematics using lattice QCD, a wealth of
information on the structure of the nucleon can be accessed. This
includes the determination of the electromagnetic form factors, the
axial form factors, moments of (generalised) parton distribution
functions and includes the gravitational form factors.... -
Evgeny Epelbaum
We review the formulations of chiral effective field theory with explicit Delta degrees of freedom and discuss the role of the Delta isobar in low-energy reactions involving pions, nucleons and photons. Topics considered include pion-nucleon scattering, pion photoproduction, Compton scattering as well as parity-conserving and parity-violating nuclear interactions.
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Dr Oleg Denisov (INFN-Torino)
It is quite evident that in order to shed a light on Emergence of Hadron Mass phenomenon it is not enough to deeply study the proton structure but to know much more about pseudoscalar mesons and excited baryons and their properties. A lack on knowledge in this field is quite justified by the fact that it is much more difficult to study properties of unstable particles (i.e. mesons and excited...
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Mr Pablo Rabán (Universidad Complutense de Madrid)
A precise description of low-energy $\pi N$ interactions and the lightest baryon spectrum is essential for many problems in hadronic and nuclear physics. Following a careful revision of the database, we determine $\pi N$ resonance parameters from forward dispersion relations using exclusively total cross-section data together with the optical theorem.
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Bianca Gualtieri (Florida International University)
Cascade hyperons, despite being discovered over half a century ago, remain considerably less studied compared to the non-strange $\Delta$ and $N$ baryons. The objective of this analysis is to provide cross-section measurements for the ground state cascade, $\Xi^-(1320)$ and $\Xi^-(1530)$ , using electron beam energies of $6.5$ and $7.5$ GeV. These measurements span both the quasi-real...
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Joannis Papavassiliou
It has long been argued that the action of the Schwinger mechanism in the gauge sector of Quantum Chromodynamics leads to the generation of a gluon mass scale. Within this scenario, the analytic structure of the fundamental vertices is modified by the creation of scalar colored excitations with vanishing mass. In the limit of zero momentum transfer,
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these terms act as massless poles,... -
Qian Wang (South China Normal University, Guangzhou, China)
Thanks to the increasing statistics of experimental data, numerous exotic candidates have been observed, such as the famous X(3872), the double charm tetraquarks, and so on In this talk, I will briefly review the current status of the study of these exotic hadrons, with a particular focus on new methods that have the potential to advance current research, such as machine learning approaches...
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Dr Stefan Diehl (Justus Liebig University Giessen and University of Connecticut)
QCD provides a rich spectrum of excited baryon states. The understanding of their internal structure is of essential important for many fields of nuclear physics, such as nuclear forces, dense matter or neutrino-nucleus interactions. It is known, that Generalized Parton Distributions (GPDs) are a well established tool for characterizing the QCD structure of the ground-state nucleon based on 3D...
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Jia-jun Wu
We present a nonperturbative Hamiltonian framework (NPHF) to address the general N-body problem. This framework rigorously connects finite-volume spectra from lattice QCD to scattering observables from experiment. Here we will present the several example to show how to use our method to extract omega from pipipi lattice spectrum.
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Arie Bodek (University of Rochester (US))
We have performed a global extraction of the 12C, 58Ca and 56Fe longitudinal (RL) and transverse (RT) nuclear electromagnetic response functions from an analysis of all available electron scattering data on these nuclei. The response functions are extracted for energy transfer spanning the nuclear excitation, quasielastic (QE), resonance and inelastic continuum over a large range of the...
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Jung Keun Ahn (Korea University)
This talk will cover the current status and future prospects of experimental searches for light pentaquark states with hadron beams, focusing on both light and hidden-flavor candidates such as $\Theta^+$ and $P_{s\bar{s}}$. Special attention will be given to upcoming experiments at the hadron hall of J-PARC and the KLF at JLab, followed by a highlight of a proposed experiment to study...
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Julia Tena Vidal (Universitat de València)
A major challenge for neutrino oscillation experiments, which rely on wide-band fluxes, is the accurate reconstruction of neutrino energy from observed final-state particles. This reconstruction depends on nuclear and interaction models embedded in event generators, which are limited by underlying assumptions and must be constrained by external data. Electron scattering experiments, which use...
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Daniel Carman (Jefferson Laboratory)
Studies of the spectrum and structure of excited nucleon ($N^*$) states via photo- and electroproduction of exclusive reactions are important for exploring non-perturbative strong interaction dynamics. Data from the $KY$ channels is complementary to studies limited to the non-strange $\pi N$, $\eta N$, and $\pi \pi N$ channels. $KY$ photoproduction observables have been pivotal in identifying...
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Zhan-Wei Liu (Lanzhou University)
We have studied nucleon and hyperon resonances based on the experimental scattering data and lattice QCD simulations within Hamiltonian effective field theory. Some of them are very exotic, for example, the is mainly a molecule and the is dynamically generated. However, the traditional triquark states are still very important and exist in the excited baryons, for example, the contains the...
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tsung-shung Lee (Argonne National Laboratory)
Using the Argonne National Laboratory-The University of Osaka (ANL-Osaka) DCC model
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of meson-nucleon reactions, we predict the cross sections of
the $\pi N \to \pi \pi N$ reactions.
The model was constructed by fitting
only the two-body reactions:
$\pi N,\gamma N \to \pi N, \eta N, K\Lambda, K\Sigma$.
Thus, the results for $\pi N \to \pi \pi N$ presented here
are predictions of the... -
Dr Hiroyuki Sako (Japan Atomic Energy Agency)
Although nucleon resonances (N and $\Delta$) have been studied for a long time, there are still many resonances which have not been established experimentally, which were measured mostly using $\gamma N\rightarrow \pi N$. $\pi N \rightarrow \pi N$, and $\gamma N \rightarrow \pi\pi N$ data. On the other hand, there are only a limited number of events of $\pi N \rightarrow \pi\pi N$ data,...
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Alexander Kvinikhidze (A. Razmadze Mathematical Institute of the Tbilisi State niversity)
In the talk a missing part of the extensively used chiral effective field theories is presented which is necessary for accurate study of the processes involving
bound states.Contemporary high precision experimental studies of the processes where bound states are involved open the possibility of the accurate study of their characteristic features. To maximise the
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accuracy the... -
Prof. Luciano Melo Abreu
We study deuteron interactions with light mesons in the hadronic phase of heavy-ion collisions. Treating the deuteron as a weakly bound state, we use the quasi-free approximation for the $d\pi$ interaction. The elementary $N\pi$ amplitudes are described by an effective model that combines the non-resonant background from chiral perturbation theory with resonant contributions parameterized by...
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Victor Mokeev (Thomas Jefferson National Accelerator Facility)
Analyses of exclusive meson electroproduction data obtained with the CLAS detector at Jefferson Lab have provided the only information on the evolution of the nucleon resonance (N) electroexcitation amplitudes—known as the γ pN* electrocouplings—over the mass range up to 1.75 GeV for photon virtualities from the photon point up to Q² = 5.0 GeV². Recent advances in these studies and their...
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Jean-Marc Richard (University of Lyon & CNRS-IN2P3, France)
We review the constituent quark model of baryons, as developed in the 1960s by Greenberg and by Dalitz and his collaborators and successors, notably Isgur and Karl, and discuss how this framework can be related to the underlying quark dynamics. We briefly address several developments beyond the simple harmonic-oscillator model, including certain mathematical aspects of the three-body problem...
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Maxim Mai (University of Bern)
What are the mechanisms behind the labyrinthine spectrum of excited hadrons? This question challenges our understanding of strong interaction and is of relevance to many applications where the exact parameters of these states influence interaction patterns.
To uncover this riddle a synergetic combination of available analytical (EFT's, S-Matrix...), Numerical (Lattice QCD), or...
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