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Barbara Erazmus17/06/2024, 09:20
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Catalina Oana Curceanu (Istituto Nazionale di Fisica Nucleare)17/06/2024, 09:30
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Fabio Bossi (Istituto Nazionale di Fisica Nucleare)17/06/2024, 09:50
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Marek Lewitowicz (GANIL)17/06/2024, 10:20
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Francesco Sgaramella (INFN-LNF)17/06/2024, 10:50
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Gert Aarts (Swansea University)17/06/2024, 11:10
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Pok Man Lo17/06/2024, 11:30
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50. Charge-conjugation asymmetry and molecular content: the Tcc(3875) and Ds(2317) in nuclear matterJuan Nieves (IFIC (CSIC-UV))17/06/2024, 12:10
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Alexandre Salas-Bernárdez (Universidad Complutense de Madrid)17/06/2024, 12:30
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Denis Veretennikov (University of the Basque Country UPV/EHU)17/06/2024, 12:50
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Mikhail Gorshteyn (Mainz University)17/06/2024, 13:10
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Tobias Fischer17/06/2024, 15:00
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Aron Kripko (JLU Gießen)17/06/2024, 15:20
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Dr Valerio Bertone (CEA Paris-Sclay)17/06/2024, 15:40
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Laboni Manna (Warsaw University of Technology)17/06/2024, 16:00
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Maria Paola Lombardo (Istituto Nazionale di Fisica Nucleare)17/06/2024, 16:20
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Andrea Zappettini17/06/2024, 17:10
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Hartmut Schmieden (Universität Bonn, Physikalisches Institut)17/06/2024, 17:30
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Paolo Lenisa (Istituto Nazionale di Fisica Nucleare)17/06/2024, 17:50
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Mikhail Gorshteyn (Mainz University)17/06/2024, 18:10
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Triloki Triloki (INFN Bari Italy)17/06/2024, 18:30
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Alessandro Scordo (Istituto Nazionale di Fisica Nucleare)18/06/2024, 09:00
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Jan Fiete Grosse-Oetringhaus (CERN)18/06/2024, 09:40
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Tetyana Galatyuk (TU Darmstadt / GSI)18/06/2024, 10:20
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Marc Vanderhaeghen (University Mainz)18/06/2024, 11:30
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Hartmut Schmieden (Universität Bonn, Physikalisches Institut)18/06/2024, 12:10
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Fuminori Sakuma18/06/2024, 12:50
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Abhay Deshpande18/06/2024, 15:00
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Gert Aarts (Swansea University)18/06/2024, 15:40
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Luciano Rezzolla (Albert Einstein Institute)18/06/2024, 16:50
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Didier Contardo18/06/2024, 17:20
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David Dobrigkeit Chinellato (Universidade Estadual de Campinas (UNICAMP))18/06/2024, 18:00
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Angels Ramos (University of Barcelona)19/06/2024, 09:00
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Aleksas Mazeliauskas (CERN Theoretical Physics Department)19/06/2024, 09:30
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Carlota Andres19/06/2024, 10:00
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Meike Küßner (Ruhr-Universität Bochum)19/06/2024, 10:30
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Barbara Pasquini (Istituto Nazionale di Fisica Nucleare)19/06/2024, 11:30
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Savvas Zafeiropoulos (CNRS and Aix Marseille University)19/06/2024, 12:00
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Stefano Forte (Istituto Nazionale di Fisica Nucleare)19/06/2024, 12:30
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Oton Vazquez Doce (Istituto Nazionale di Fisica Nucleare)19/06/2024, 13:00
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Graziano Venanzoni (Istituto Nazionale di Fisica Nucleare)19/06/2024, 15:00
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Piergiorgio Cerello (Istituto Nazionale di Fisica Nucleare)19/06/2024, 15:30
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19/06/2024, 16:30
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19/06/2024, 16:45
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Dr Valerio Bertone (CEA Paris-Sclay)
The need for efficient and accurate numerical codes to study the 3D structure of hadrons is today more than ever an essential requirement. In this respect the virtual-access (VA) packages of STRONG2020 have played a leading role. In this contribution, we will present the latest achievements of the 3DPartons VA package of STRONG2020. On top of the code developments accomplished over the past...
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Andrea Dainese (Istituto Nazionale di Fisica Nucleare)
The ALICE Collaboration proposes a completely new apparatus, ALICE 3, for the LHC Runs 5 and 6 (arXiv:2211.02491). The detector consists of a large pixel-based tracking system covering eight units of pseudorapidity, complemented by multiple systems for particle identification, including silicon time-of-flight layers, a ring-imaging Cherenkov detector, a muon identification system, and an...
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Tobias Fischer
Motivated from the observations of poorly understood explosive stellar phenomena associated with massive supergiant stars of zero-age main sequence (ZAMS) masses around 30–60 solar masses, new light has been shed on an old idea [1], namely, that the appearance of QCD degrees of freedom may account for such cosmic explosions [2]. Obeying nuclear physics constraints and taking yet another...
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Andrea Zappettini
In this work, we will present the potentialities of new quasi-hemispherical CdZnTe (CZT) detectors, recently developed at IMEM- CNR Parma (Italy), for high-resolution X-ray spectroscopy of intermediate mass kaonic atoms. Among the possible single-polarity electrode configurations, such as coplanar, pixelated, or virtual Frisch-grid geometries, quasi-hemispherical detectors are the most...
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39. Charge-conjugation asymmetry and molecular content: the Tcc(3875) and Ds(2317) in nuclear matterJuan Nieves (IFIC (CSIC-UV))
We analyze the modifications that a dense nuclear medium induces in the Ds(2317)± and Tcc(3875)±. In the vacuum, we consider them as isoscalar DK (Dbar Kbar) and DD (Dbar Dbar) S-wave bound states, which are dynamically generated from effective interactions that lead to different Weinberg compositeness scenarios. Matter effects are incorporated through the two-meson loop functions, taking into...
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Mikhail Gorshteyn (Mainz University)
A relativistic beam of partially-stripped ions can be irradiated with a laser whose frequency is tuned to a resonant atomic transition which will subsequently de-excite. This mechanism allows one to obtain a $\gamma$-source of an unprecedented brilliance and intensity. The Gamma Factory proposed at the LHC is able to produce up to $10^{18}$ photons per second (7 orders of magnitude beyond the...
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Aron Kripko (JLU Gießen)
A multidimensional study of the structure function ratio $\mathrm{F_{LU}^{sin(\phi)}/F_{UU}}$ has been performed for pion and charged kaon semi-inclusive deeply inelastic scattering (SIDIS), based on the measurement of beam-spin asymmetries. It uses the high statistics data recorded with the CLAS12 spectrometer at Jefferson Laboratory. The 10.6 GeV longitudinally polarized electron beam...
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Laboni Manna (Warsaw University of Technology)
In this talk, I will present our extensions of MadGraph5_aMC@NLO for two
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asymmetric systems, photoproduction and proton-nucleus collisions, as well as progress towards automation of computations for inclusive-quarkonium production, currently being worked out at leading order.
Indeed, to consolidate the figures of merit of a variety of measurements at the Electron-Ion Collider and systematise... -
Gert Aarts (Swansea University)
As the temperature increases, hadrons are expected to be affected and eventually dissolve or melt into deconfined quarks and gluons. I'll review some of the work done using lattice QCD on the behaviour of hadrons under increasing temperature, focussing on activities of the FASTSUM collaboration.
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Francesco Sgaramella (INFN-LNF)
The low-energy QCD, the theory within the Standard Model describing the strong interaction, is still missing fundamental experimental results to achieve a breakthrough in its understanding. Among these experimental results, kaonic atoms X-ray spectroscopy represents a unique laboratory for the study of the antikaon-nucleon/nuclei interaction at threshold energy, with important consequences...
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Maria Paola Lombardo (Istituto Nazionale di Fisica Nucleare)
LaVA is established within the STRONG-2020 project, with the support of FBK/ECT* and INFN, with the aim of providing an advanced and inclusive tool for training in Lattice Field Theory. The scientific management is done by the LatticeHadrons Network of Strong-2020 , with the support of an invited Advisory Board comprising leading scientists in the field.
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A Beta version of the site is... -
Alessandro Scordo (Istituto Nazionale di Fisica Nucleare)
The INFN Laboratories of Frascati (LNF) are a very sparkling laboratory.
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Thanks to already existing and planned high-quality infrastructures, they
represent an ideal environment to perform Hadron Physics experiments.
The main infrastructure is the DAFNE e+e- collider, where several crucial
activities and experiments have been already performed in the strangeness
sector. In particular, the... -
Paolo Lenisa (Istituto Nazionale di Fisica Nucleare)
Two of the major scientific drivers of particle physics and cosmology are the faith of antimatter after the Big Bang and the origin of Dark Matter. The answers to these questions can be addressed by investigating permanent and oscillating Electric Dipole Moments (EDM) of fundamental particles. The experiments can be performed with polarized beams in a dedicated storage ring.
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Important... -
Prof. Angels Ramos (University of Barcelona)
In this talk I will review the recent developments on strangeness hadron physics, covering aspects of the elementary interactions of kaons and hyperons with nucleons and nuclei. I will also discuss the impact of strange particles in astrophysical contexts, analyzing their role in the properties of neutron stars and in the characteristics of gravitational waves produced during binary neutron...
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Denis Veretennikov (University of the Basque Country UPV/EHU)
The HERMES experiment has collected a wealth of data using the 27.6 GeV longitudinally polarized HERA lepton beam and various polarized and unpolarized gaseous targets. This allows for a series of unique measurements of observables sensitive to the multidimensional (spin) structure of the nucleon, in particular semi-inclusive deep-inelastic scattering (SIDIS) measurements, for which the HERMES...
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Alexandre Salas-Bernárdez (Universidad Complutense de Madrid)
Phenomenological evidence suggests that strong decays of low-excitation hadrons often involve the creation of a light quark-antiquark pair with zero angular momentum, known as the $^3P_0$ mechanism, derived from a scalar bilinear. Despite Quantum Chromodynamics being mediated perturbatively by spin-one gluons and exhibiting chiral symmetry in its Lagrangian, a scalar decay term appears...
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Hartmut Schmieden (Universität Bonn, Physikalisches Institut)
The discovery of the X, Y, Z states in the (hidden) charm meson sector first by Belle, and the P_C baryon states by LHCb revealed the existence of multi-quark objects beyond the simple quark-antiquark or 3-quark valence configurations. If the emergence of such multi-quark structures was a general feature of QCD, then related structures should exhibit in the uds-sector as well. The BGOOD...
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Pok Man Lo
I shall present an analysis of the thermal composition of the S=-1 strange baryons using an S-matrix formulation of statistical mechanics. The thermal abundances are computed based on the density of states extracted from a coupled-channel model. The approach entails a consistent treatment of resonances and naturally incorporates nonresonant interactions and the contribution from some...
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