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Swati Saha (IIT- Indian Institute of Technology (IN))13/04/2026, 09:10
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Marvin Nabroth13/04/2026, 09:40
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Seweryn Kowalski (University of Silesia (PL))13/04/2026, 10:10
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Dr Fan Si (Heidelberg University (DE))13/04/2026, 11:00
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Piotr Gasik (GSI - Helmholtzzentrum fur Schwerionenforschung GmbH (DE))13/04/2026, 11:30
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Giacomo Alocco (Universita e INFN, Torino (IT))13/04/2026, 12:00
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Charles Joseph Naim13/04/2026, 14:00
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Patrycja Anna Potepa (AGH University of Krakow (PL))13/04/2026, 14:20
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Dr Georgios Krintiras (The University of Kansas (US))13/04/2026, 14:40
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Imanol Corredoira (Université Paris-Saclay (FR))13/04/2026, 15:00
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Jana N. Guenther (University of Wuppertal)13/04/2026, 15:50
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Prof. Wei-jie Fu (Dalian University of Technology)13/04/2026, 16:20
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Dr Anar Rustamov (GSI Helmholtzzentrum für Schwerionenforschung GmbH)13/04/2026, 16:50
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Larry McLerran13/04/2026, 17:20
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Leonid Glozman14/04/2026, 09:00
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Noriyuki Sogabe14/04/2026, 09:20
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Dr Aleksas Mazeliauskas14/04/2026, 09:40Oral
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Jannis Gebhard (Heidelberg University)14/04/2026, 10:00
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Shi Yin (Institute for Theoretical Physics, Justus Liebig University Giessen)14/04/2026, 10:20
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Dibyendu Bala (Bielefeld University)14/04/2026, 11:00
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Peter Braun-Munzinger (GSI - Helmholtzzentrum fur Schwerionenforschung GmbH (DE))14/04/2026, 11:30
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Mr Tribhuban Parida (AGH UST Krakow)14/04/2026, 12:00
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Dr Yi Yin (Chinese University of Hong Kong (Shenzhen))14/04/2026, 12:20
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Mr Rutik Manikandhan (University of Houston)14/04/2026, 14:00
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Prof. Gokce Basar (University of North Carolina, Chapel Hill)14/04/2026, 14:20
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Dr Johannès Jahan (University of Houston - Department of Physics)14/04/2026, 14:50
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Jianing Li14/04/2026, 15:20
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Ke Mi (University of Chinese Academy of Sciences / Central China Normal University)14/04/2026, 16:10
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Oleksii Ivanytskyi (University of Wroclaw)14/04/2026, 16:30
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Agnieszka Sorensen (Institute for Nuclear Theory), Agnieszka Sorensen (University of Washington)14/04/2026, 16:50
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Andrzej Krzysztof Rybicki (Polish Academy of Sciences (PL))14/04/2026, 17:20
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Jamie Karthein (MIT), Dr Jamie Karthein (MIT)15/04/2026, 09:00
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Xin Dong15/04/2026, 09:30
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Marvin Nabroth15/04/2026, 10:00
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Ashish Pandav15/04/2026, 10:20
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Mario Ciacco (Universita and INFN Torino (IT))15/04/2026, 11:10
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Oleksandra Panova (Institute of Nuclear Physics Polish Academy of Sciences (PL))15/04/2026, 11:30
NA61/SHINE is a multipurpose fixed-target experiment located at the CERN SPS. One of its main goals is to study the onset of deconfinement and the properties of strongly interacting matter. For this purpose, a unique two-dimensional scan in collision energy (√sNN = 5.1 − 16.8/17.3 GeV) and system size was performed.
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Results on hadron spectra produced in nucleus-nucleus collisions, including... -
Piyush Kumar (University of Wuppertal)15/04/2026, 11:50
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Szabolcs Istvan Borsanyi15/04/2026, 12:10
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Guangyu Zheng (University of Chinese Academy of Sciences)15/04/2026, 12:30Oral
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Yige Huang15/04/2026, 14:00
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Barnabas Porfy (HUN-REN Wigner Research Centre for Physics (HU))15/04/2026, 14:20
The NA61/SHINE experiment at the CERN SPS is a multipurpose fixed-target spectrometer for charged and neutral hadron measurements. Its research program includes strong interaction studies focusing on the exploration of the QCD phase diagram and understanding the phase structures of strongly interacting matter, including the hypothesized QCD critical point. To map the QCD phase diagram, the...
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Zhaohui Wang (Central China Normal University)15/04/2026, 14:40
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Franz Richard Sattler (University Bielefeld)15/04/2026, 15:00
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Rudrapriya Das (Bose Institute)15/04/2026, 15:20
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Nu Xu (Lawrence Berkeley National Lab. (US))15/04/2026, 15:40
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Michael Doser (Massachusetts Inst. of Technology (US))15/04/2026, 16:30
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Reyes Alemany Fernandez (CERN)15/04/2026, 16:50
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Marianna Mazzilli (Universita e INFN, Bari (IT))15/04/2026, 17:10
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Kevin P. Pala16/04/2026, 09:00
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Francesco Di Clemente (University of Houston)16/04/2026, 09:20
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Xin An (Ghent University)16/04/2026, 09:40
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Thomas Schaefer16/04/2026, 10:00
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Szymon Harabasz16/04/2026, 10:50
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Ms Iuliana-Carina Udrea (Technische Universität Darmstadt)16/04/2026, 11:10
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Jessica Ou Ya Vogel16/04/2026, 11:30
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Renan Góes-Hirayama (FIAS)16/04/2026, 11:50
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Mr Behruz Kardan (IKF, Uni-Frankfurt)16/04/2026, 12:10
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Vojtěch Honěk (FNSPE, CTU in Prague)16/04/2026, 14:00
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Boris Tomasik16/04/2026, 14:20
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Dr Volodymyr Vovchenko (University of Houston)16/04/2026, 14:40
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Antoni Marcinek (Polish Academy of Sciences (PL))16/04/2026, 15:00
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Iris Ponce (Yale University)16/04/2026, 15:20
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Nicolò Jacazio (Universita del Piemonte Orientale (IT))16/04/2026, 15:40
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Nu Xu (Lawrence Berkeley National Lab. (US)), Dr Yi Yin (Chinese University of Hong Kong (Shenzhen))17/04/2026, 09:00
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Gregoire Marvin Nelson Pihan (University of Houston)17/04/2026, 09:10
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Dr Iurii Karpenko (FNSPE CTU in Prague)17/04/2026, 09:40
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Liubing Chen (Central China Normal University)17/04/2026, 10:10
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Ludovica Pirelli (Bergische Universität Wuppertal)17/04/2026, 10:30
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Jishnu Goswami (Bielefeld University)17/04/2026, 11:20
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Dr Volodymyr Vovchenko (University of Houston)17/04/2026, 11:40
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Reyes Alemany Fernandez (CERN)Oral
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Marianna Mazzilli (Universita e INFN, Bari (IT))Future ExperimentsOral
The ALICE Collaboration has proposed a new detector concept, ALICE 3, for LHC Run 5 (LoI, arXiv:2211.02491). The detector features a large pixel-based tracking system covering a wide range in pseudorapidity, complemented by advanced particle-identification subsystems, including silicon time-of-flight layers and a ring-imaging Cherenkov detector. A retractable vertex detector installed inside...
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Adam Bzdak (AGH University of Science and Technology)Critical PointOral
In this talk, I will present our study [1] on joint factorial cumulants of protons and antiprotons in relativistic heavy-ion collisions. We find that if the correlations in the system arise solely from long-range effects, such as global baryon conservation and volume fluctuations, these cumulants should follow a universal scaling with acceptance. The STAR results from phase I of the RHIC Beam...
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Gregoire Marvin Nelson Pihan (University of Houston)
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Noriyuki SogabePhase TransitionOral
At the last CPOD meeting, STAR reported Beam Energy Scan (BES)-II baryon cumulant data that exhibit a non-monotonic dependence on collision energy, suggesting critical behavior. Identifying signatures of the associated first-order chiral phase transition would complement these fluctuation measurements and help establish a more robust picture of the phase structure at high baryon density.
To...
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Dr Volodymyr Vovchenko (University of Houston)HadronizationOral
We develop a general framework for event-by-event fluctuations and correlations of hadron numbers in statistical hadronization with exact conservation of multiple charges, building on the density–correlation formalism of Refs. [1,2]. The approach incorporates local charge conservation and microscopic particle correlations, including excluded-volume effects, baryon–antibaryon annihilation,...
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Liubing Chen (Central China Normal University)HadronizationOral
Author: Liubing Chen
Charged pion production in heavy-ion collisions at energies of a few GeV per nucleon pair is essential for exploring the bulk properties and equation of state of QCD matter in the high baryon density regime. The STAR experiment at RHIC has conducted a comprehensive Beam Energy Scan from $\sqrt{s_{\mathrm{NN}}} = 13.7~\mathrm{GeV}$ down to $\sqrt{s_{\mathrm{NN}}} =...
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Jessica Ou Ya VogelPhase TransitionOral
Measurements of dileptons emitted from heavy-ion collisions provide insights into the properties of the created fireball. As leptons are unaffected by strong final-state interactions, they carry valuable information about the hot and dense medium formed in the early stages of the collision. The high baryon densities achieved in heavy-ion reactions at a few GeV induce significant medium effects...
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Ms Agnieszka Sorensen (University of California, Los Angeles), Agnieszka Sorensen (University of Washington), Agnieszka Sorensen (Institute for Nuclear Theory)Oral
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Francesco Di Clemente (University of Ferrara), Dr Johannès Jahan (University of Houston - Department of Physics)Critical PointOral
Recently, a new equation of state based on the two-dimensional T'-expansion scheme with a parametrizable critical point from the 3D Ising model was released. It allows to produce a family of equations of state which can be used to study the effect of critical point in the QCD phase diagram, primordial to infer its existence and location from experimental results. Employing the newly developed...
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Vojtěch Honěk (FNSPE, CTU in Prague)HadronizationOral
We calculate the BQ susceptibility of an interacting hadron gas an non-vanishing baryon density. The pion-nucleon interation is accounted for with the help of S-matrix. The susceptibility largely increases when the chemical potential grows. We show the results evaluated along the chemical freeze-out line, which provides non-critical reference for this observable. Also, we study the evolution...
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Vojtěch Honěk (FNSPE, CTU in Prague)
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Manjunath Omana Kuttan (Frankfurt Institute for Advanced Studies)Future ExperimentsOral
Relativistic heavy-ion collisions at GSI, FAIR, RHIC-BES, and HIAF probe the phase structure of QCD matter at moderate temperatures and high densities, where first-principles calculations are infeasible and systematic model-to-data comparison techniques such as Bayesian inference are the norm to extract the underlying physics. However, the computational cost of model simulations limits the use...
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Manjunath Omana Kuttan (Frankfurt Institute for Advanced Studies)
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Guangyu Zheng (University of Chinese Academy of Sciences)Oral
This talk will present the energy dependence of proton $v_3$ with respect to the first-order event plane, determined using the Event Plane Detector, as measured by STAR in Au+Au collisions at center-of-mass energies between 3 and 4.5 GeV. Models indicate that $v_3(\psi_1)$ at these energies is generated not by fluctuations but by the collision geometry produced by a combination of nuclear...
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Shi Yin (Institute for Theoretical Physics, Justus Liebig University Giessen)Phase TransitionOral
Dense QCD matter can feature a moat regime, where the static energy of mesons is minimal at nonzero momentum. Valuable insights into this regime can be gained using low-energy models. This, however, requires a careful assessment of model artifacts. We therefore study the effects of renormalization and in-medium modifications of quark-meson interaction on the moat regime. To capture the main...
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Marvin NabrothCritical PointOral
Experimental studies of QCD matter at extreme densities and moderate temperatures are made possible through low-energy heavy-ion collisions. At SIS18/GSI, the HADES experiment (High-Acceptance Dielectron Spectrometer) is optimized to reconstruct reaction products from heavy-ion collisions at kinetic beam energies of about 1 AGeV, enabling the investigation of freeze-out conditions at the...
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Marvin Nabroth
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Szymon HARABASZ, Szymon Harabasz, Szymon HarabaszOral
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Boris Tomasik (Czech Technical University in Prague (CZ))HadronizationOral
There is ongoing debate about the production mechanism of deuterons. Statistical production seems to describe the yields well, but seems unlikely on the short time scales of the collisions, as the binding energy of the deuteron is much smaller than the typical temperature of the producing hot fireball. The alternative is offered by coalescence. We propose that the two mechanisms could be...
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Xin DongOral
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Charles Joseph NaimOral
The ePIC detector at the future Electron–Ion Collider (EIC) at Brookhaven National Laboratory will be one of the most advanced tools to explore the structure of hadronic matter at small Bjorken-x. By probing protons and nuclei with unprecedented precision, the EIC will open new territories of Quantum Chromodynamics (QCD). Beyond its collider mission, the EIC should be seen as a multi-purpose...
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Mr Behruz Kardan (IKF, Uni-Frankfurt)Phase TransitionOral
Heavy-ion collisions in the few-GeV energy range create strongly interacting matter at extreme baryon densities, comparable to those in neutron star mergers. Precise measurements of the Equation-of-State of this kind of matter in this regime are therefore essential for the understanding of neutron stars.
We present new results from HADES (High-Acceptance Dielectron Spectrometer) located...
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Prof. Wei-jie Fu (Dalian University of Technology)Oral
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Kevin P. PalaCritical PointOral
The Quark–Gluon Plasma has been created and studied for decades in relativistic heavy-ion collisions. Still, a central question remains open: whether a critical point exists in the QCD phase diagram and where it lies. At top RHIC and LHC energies, the system probes high temperature and nearly zero baryon chemical potential. Exploring finite-density regions requires lower energies and dedicated...
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Antoni Marcinek (Polish Academy of Sciences (PL))Deconfined MatterOral
NA61/SHINE is a multipurpose, fixed-target hadron spectrometer at the CERN SPS. Its research program includes studies of strong interactions as well as reference measurements for neutrino and cosmic-ray physics. A significant advantage of NA61/SHINE over collider experiments is its extended coverage of phase space available for particle production. This includes the entire projectile...
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Renan Góes-Hirayama (FIAS)Phase TransitionOral
We calculate dielectron yields for different equations of state at beam energies relevant for the CBM experiment at FAIR and the STAR Beam energy Scan. The production of dielectrons of intermediate masses ($1<m_{ee}/\mathrm{GeV}<3$) is increased by the presence of a phase transition, due to the latent heat. In this work, we quantify this enhancement using a hybrid model of hadronic...
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Jishnu Goswami (Bielefeld University)Critical PointOral
QCD material parameters, such as the speed of sound, isothermal compressibility, and thermal expansion coefficient, quantify how soft the equation of state (EOS) is at finite temperature and chemical potentials. To understand the nature of the hot and dense matter created in heavy-ion collision experiments, we contrast experimental measurements with first-principles lattice QCD calculations at...
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Peter Braun-Munzinger (GSI - Helmholtzzentrum fur Schwerionenforschung GmbH (DE))
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Dr Iurii Karpenko (FNSPE CTU in Prague)Oral
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Franz Sattler (University Bielefeld)Critical PointOral
QCD at large densities exhibits a moat regime in the scalar-pseudoscalar sector. The resolution of its dynamics is pivotal for the access to the onset of new phases including the potential critical endpoint of QCD. I report on a first self-consistent analysis of this regime, using the functional Renormalisation Group approach to QCD.Mapping out the moat regime, we find a potential...
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Mr Tribhuban Parida (AGH UST Krakow)Deconfined MatterOral
Two central objectives of the Beam Energy Scan (BES) program at RHIC are the identification of signatures of critical fluctuations and the extraction of electromagnetic (EM) field effects. However, the lack of reliable baseline predictions hampers both efforts. In hydrodynamic modeling, this limitation arises primarily from the absence of a realistic description of baryon deposition that can...
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Andrzej Krzysztof Rybicki (Polish Academy of Sciences (PL)), Seweryn Kowalski (University of Silesia (PL))HadronizationOral
NA61/SHINE at the CERN SPS is a multipurpose fixed-target detector for charged and neutral hadron measurements. The research program of the experiment includes studies of strong interactions as well as reference measurements for neutrino and cosmic-ray physics. A significant advantage of NA61/SHINE over collider experiments is its extended coverage of phase space available for hadron...
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Christian Schmidt-SonntagCritical PointOral
We report on the status of Lee-Yang edge singularity calculations in Lattice QCD. In particular we discuss possibilities to improve systematical and statistical errors of the results presented in [1], from where we find a possible QCD critical end point (CEP) located at $𝑇^{CEP} =102^{+11}_{−23} $ MeV and $𝜇_B^{CEP} =428^{+162}_{−74}$ MeV. We improve our previous calculation by doubling the...
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Christian Schmidt-Sonntag
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Ms Iuliana-Carina Udrea (Technische Universität Darmstadt)Phase TransitionOral
Understanding the QCD phase structure at high net-baryon density and moderate temperature is uniquely accessible through dilepton measurements with HADES at SIS18 operating in GSI.
Virtual photons (dileptons) serve as a penetrating probe that gives direct insight into the electromagnetic emissivity of the hot and dense medium. This makes them a unique tool for exploring the microscopic...
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Zhaohui Wang (Central China Normal University)Critical PointOral
Fluctuations of conserved quantities are proposed as sensitive observables to search for the QCD critical point in heavy-ion collisions. Recently, the STAR experiment has conducted precision measurement of net-proton fluctuations in Au+Au collisions at $\sqrt{s_{NN}}$ = 7.7 – 27 GeV, during the RHIC Beam Energy Scan II program [1] and reported the preliminary results of proton number...
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Zhangwei Zheng (University of Chinese Academy of Sciences)HadronizationOral
The high-baryon-density region provides a unique opportunity to explore the QCD phase structure and the role of strange quarks in hadronic interactions. Previous correlation measurements of $p$-$\Lambda$ and $p$-$\Xi$ suggest that the strange degree of freedom may weaken hadronic interactions. Experimentally, the directed flow ($v_1$) of $\phi$ mesons in this environment exhibits baryon-like...
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Zhangwei Zheng (University of Chinese Academy of Sciences)
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Michael Doser (Massachusetts Inst. of Technology (US))Oral
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Giacomo Alocco (Universita e INFN, Torino (IT))Oral
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Swati Saha (National Institute of Science Education and Research (NISER) (IN)), Swati Saha (National Institute of Science Education and Research (NISER) (IN))Oral
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Oral
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Dr Georgios Krintiras (The University of Kansas (US))Oral
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Oral
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Dr Johannès Jahan (University of Houston - Department of Physics)Oral
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Seweryn Kowalski (University of Silesia (PL))Oral
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Oral
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Barnabas Porfy (HUN-REN Wigner Research Centre for Physics (HU)), Dr Nikolaos Davis (Institute of Nuclear Physics, Polish Academy of Sciences (PL))Critical PointOral
The NA61/SHINE experiment at the CERN SPS is a multipurpose fixed-target spectrometer for charged and neutral hadron measurements. Its research program includes strong interactions studies focusing on the exploration of the QCD phase diagram and understanding the phase structures of strongly interacting matter, including the hypothesized QCD critical point. To achieve these goals, the...
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Oleksandra Panova (Jan Kochanowski University (PL)), Yuliia Balkova (National Centre for Nuclear Research (PL))Phase TransitionOral
NA61/SHINE is a multipurpose fixed-target experiment located at the CERN SPS. One of its main goals is to study the onset of deconfinement and the properties of strongly interacting matter. For this purpose, a unique two-dimensional scan in collision energy (√sNN = 5.1 − 16.8/17.3 GeV) and system size was performed.
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Results on hadron spectra produced in nucleus-nucleus collisions, including... -
Mr Rutik Manikandhan (University of Houston)Critical PointOral
We report the first measurements of two-particle transverse momentum correlations for mid-rapidity charged particles in Au+Au collisions at $\sqrt{s_{\rm NN}} =$ 3.0–7.7 GeV recorded by the STAR experiment from the Beam Energy Scan Phase-II (BES-II). The results are compared with previous STAR measurements from BES-Iand with transport model calculations. The measured two-particle $p_{\rm T}$...
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Prof. Gokce Basar (University of North Carolina, Chapel Hill)Oral
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Krzysztof Redlich (GSi Darmstadt), Krzysztof Redlich (National Centre for Nuclear Research (PL)), Krzysztof Redlich (University of Wroclaw)Oral
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Ludovica Pirelli (Bergische Universität Wuppertal)Oral
Finite density lattice QCD usually relies on extrapolations in baryon
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chemical potential ($\mu_{B}$), be it Taylor expansion, T' expansion
or analytical continuation. However, their range of validity is difficult
to control. In the canonical formulation, the baryon density is the
parameter of the system, not $\mu_{B}$. Here we demonstrate that
we can access finite density QCD in the... -
Rudrapriya Das (Bose Institute)Critical PointOral
The proposed Compressed Baryonic Matter (CBM) experiment at the Facility for Antiproton and Ion Research (FAIR), Darmstadt, Germany is going to offer a unique opportunity to study the model-predicted first-order phase transition between the hadronic phase to the Quark-Gluon Plasma (QGP) phase with high precision. This will be enabled by its exceptionally high interaction rate capability—up to...
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Yige HuangCritical PointOral
The study of fluctuations and correlations of conserved charges in heavy-ion collisions offers unique insight into the QCD phase structure and serves as a promising tool to probe the critical behavior.
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Studying how fluctuations behave within different sub-volume offers an effective way to explore the critical dynamics.
Finite-size scaling based on rapidity-window selection allows one to... -
Ke Mi (University of Chinese Academy of Sciences / Central China Normal University)Compact StarsOral
The study of multi-baryon interactions, particularly those involving strange quarks, is key to understanding dense nuclear matter and the equation of state of neutron stars. While two-body nucleon-nucleon ($N$-$N$) and hyperon-nucleon ($Y$-$N$) forces are relatively well constrained, genuine three-body interactions remain largely unexplored. Comparing systems with only nucleons to those...
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Heng-Tong DingCritical PointOral
At finite baryon density, the nature of the QCD crossover and the possible existence of a critical endpoint (CEP) depend on which universality class governs the transition. In the analytic description of QCD thermodynamics in the complex $\mu_B$ plane in terms of Lee--Yang zeros, the crossover transition on the real $\mu_B$ axis is controlled by the Lee--Yang edge singularity closest to that...
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Heng-Tong Ding
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Piyush Kumar (University of Wuppertal)Phase TransitionOral
Mapping the phase diagram of Quantum Chromodynamics (QCD) at large density is a challenging task due to the complex action problem in lattice simulations. Through simulations at imaginary baryon chemical potential $\mu_B$ we observe that, if the strangeness neutrality condition is imposed, both the strangeness chemical potential $\mu_S/\mu_B$ and the strangeness susceptibility $\chi_2^S$ take...
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Jana N. Guenther (University of Wuppertal)Oral
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Larry McLerran, Larry McLerran (BNL), Larry McLerranOral
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Thomas SchaeferCritical PointOral
We describe recent results obtained from numerical simulations
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of stochastic fluid dynamics near a QCD critical point. We
discuss results for the dynamic critical exponent, the
critical behavior of transport coefficients, and the relaxation
rate of equal-time correlation functions. We also discuss
some exploratory studies of stochastic relativistic fluid
dynamics. -
Oleksii Ivanytskyi (University of Wroclaw)Compact StarsOral
We apply recently proposed three-flavor nonlocal NJL model of quark matter with the scalar attractive, vector repulsive and diquark pairing interaction channels to study the isospin dependence of the quark deconfinement and to establish the correspondence between the quark onset densities typical for heavy ion collisions and neutron stars. The model provides qualitative agreement with the...
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Ashish PandavCritical PointOral
Fluctuations of charged-particle multiplicities are sensitive observables proposed to probe the Quantum Chromodynamics (QCD) phase structure, such as searching for a possible critical point at high baryochemical potential ($\mu_B$), where enhanced fluctuations are theoretically expected. Recent measurements of proton multiplicity fluctuations across the $\sqrt{s_{NN}} = 3$–27 GeV range in...
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Vinh Luong (Joint Institute for Nuclear Research)HadronizationOral
Measurements of identical pion femtoscopy offer insights into collision dynamics, such as collective expansion, geometry of the collision zone at freeze-out, final state interactions, etc. In addition to the quantum interference and Coulomb interactions among the pion pairs, Coulomb interactions between the pair and the net positive charge in the emitting source affect the final correlation...
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Mario Ciacco (Universita and INFN Torino (IT))Phase TransitionOral
Lattice QCD calculations predict the existence of a crossover between a deconfined, thermalised partonic phase and the hadronic phase under conditions of exact baryon–antibaryon symmetry. Fourth-order baryon-number susceptibilities show significant deviations from the hadron resonance gas across the crossover, carrying information on residual criticality associated with the chiral phase...
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Iris Ponce (Yale University)Deconfined MatterOral
The study of high-energy collisions of small systems has generated
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significant discussions about the initial conditions, including the size of the system, needed to generate a Quark-Gluon Plasma (QGP). Results from asymmetric small systems, such as p+Au and p+Pb, exhibit some QGP-like signatures (e.g., flow and enhancement of strangeness production) but not others (e.g., jet quenching).... -
Dr Aleksas Mazeliauskas (Heidelberg University (DE)), Derek TeaneyPhase TransitionOral
We discuss the universal non-equilibrium enhancement of long-wavelength Goldstone bosons induced by quenches to broken phase in Model G -- the dynamical universality class of an O(4)-antiferromagnet and chiral QCD phase transition. Generic scaling arguments predict a parametric enhancement in the infrared spectra of Goldstones, which is confirmed by fully-fledged stochastic simulations. The...
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Dr Aleksas Mazeliauskas (Heidelberg University (DE)), Derek Teaney, Jannis Gebhard (Heidelberg University)Phase TransitionOral
High-energy heavy-ion collisions create a quark–gluon plasma (QGP) with approximately restored chiral symmetry. Lattice QCD determines the chiral crossover temperature to be $T_c = (156.5 \pm 1.5) \, \mathrm{MeV}$, below which chiral symmetry is spontaneously broken and pions emerge as pseudo–Goldstone bosons. Yet, this chiral transition—second order in the chiral limit—is absent from current...
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Nicolò Jacazio (Universita del Piemonte Orientale (IT))Deconfined MatterOral
Recent measurements in pp and p--Pb collisions at the LHC showed that the production of light-flavour hadrons relative to pions increases with the charged particle multiplicity of the event already in small systems.
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This smooth evolution connects different collision systems almost independently of the collision energy.
It is also observed in the strangeness sector, where the increased... -
Jamie Karthein (MIT), Dr Jamie Karthein (MIT)Oral
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Leonid GlozmanPhase TransitionOral
I discuss three different regimes/phases of QCD at high T.
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They differ by symmetries and Nc scaling. At low T until
chiral restoration temperature Tch ~ 155 MeV we have a hadron gas with
confinement and spontaneously broken chiral symmetry. The scaling
of energy density, pressure and entropy density is Nc⁰. Above
Tch and below the deconfinement temperature, Td ~ 300 MeV, QCD
is chirally... -
Xin An (Ghent University)Critical PointOral
Relativistic hydrodynamics has been remarkably successful in describing the evolution of the quark–gluon plasma created in heavy-ion collisions. To capture event-by-event fluctuations in observables—particularly those sensitive to the QCD critical point—a fully relativistic framework for non-linear fluctuating hydrodynamics is required. In this work, we construct such a framework by...
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Dr Yi Yin (Chinese University of Hong Kong (Shenzhen))Deconfined MatterOral
The Second Beam Energy Scan (BES-II) data from RHIC offers a unique opportunity to constrain the QCD EoS in the high-baryon-density region. Utilizing this opportunity requires dynamical modeling with a parametrized EoS as input.
We propose a new parametrization scheme, called physics-informed parametrization, based on the assumption that the QCD EoS can be mapped onto an artificial spin...
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Dibyendu Bala (Bielefeld University)Oral
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Jianing Li (Heidelberg University)Critical PointOral
Cumulants of net-baryon number fluctuations have been widely used as sensitive probes of the QCD critical point. However, these fluctuations are influenced not only by critical dynamics but also by global conservation of net baryon number, since the QGP fireball created in heavy-ion collisions is effectively an isolated system. In this talk, we propose a rapidity-dependent analysis based on...
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Szabolcs Istvan BorsanyiOral
We present first results from a density-of-states-based new simulation
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approach to finite density lattice QCD. We mitigate the overlap problem of
Taylor extrapolations to a degree, that the finite density transition can
be studied, including densities and fluctuations near the chiral crossover
at and beyond $\mu_B$=500 MeV. We compute the partition function, not its
logarithm, and thus... -
Szabolcs Istvan Borsanyi
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