Contribution List

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  1. 16/11/2026, 08:00
  2. Zuo-tang Liang
    16/11/2026, 08:30
  3. Zhenyu Chen (Shandong University)
    16/11/2026, 09:00
  4. Prof. Xiaoming Zhang (Central China Normal University)
    16/11/2026, 09:30
  5. Kenji Fukushima (The University of Tokyo)
    16/11/2026, 10:30
  6. Jinfeng Liao (Indiana University Bloomington)
    16/11/2026, 11:00
  7. Xu-Guang Huang (Fudan University)
    16/11/2026, 11:30
  8. Qiye Shou (Fudan University)
    16/11/2026, 12:00
  9. Francesco Becattini (Università di Firenze)
    16/11/2026, 14:00
  10. Defu Hou (CCNU)
    16/11/2026, 14:30
  11. 建华 高 (山东大学(威海))
    16/11/2026, 15:00
  12. Dr Xin-Li Sheng (INFN Florence )
    16/11/2026, 15:30
  13. Koichi Hattori (Zhejiang University)
    16/11/2026, 16:30
  14. 梓岳 王 (Tsinghua Univerisity)
    16/11/2026, 17:00
  15. Andrea Palermo
    16/11/2026, 17:30
  16. Daniele Roselli (University of Florence)
    16/11/2026, 18:00
  17. Xin-Nian Wang (Central China Normal University)
    17/11/2026, 08:30
  18. Jiangyong Jia (Stony Brook University)
    17/11/2026, 09:00
  19. Cong Yi (USTC)
    17/11/2026, 09:30
  20. Dirk Rischke (Goethe University Frankfurt am Main)
    17/11/2026, 10:30
  21. Fuqiang Wang (Huzhou University)
    17/11/2026, 11:00
  22. Jinhui Chen (Fudan University)
    17/11/2026, 11:30
  23. KaiJia Sun (Institute of Modern Physics, Fudan University)
    17/11/2026, 12:00
  24. Huan Zhong Huang (Fudan University/UCLA)
    17/11/2026, 14:00
  25. Heng-Tong Ding (Central China Normal University)
    17/11/2026, 14:30
  26. Eduardo Garnacho-Velasco (Eotvos Lorand University)
    17/11/2026, 15:00
  27. Prof. xinyang wang (Anhui University of Science & Technology)
    17/11/2026, 15:30
  28. Prof. Igor Ivanov (SYSU, School of Physics and Astronomy)
    17/11/2026, 16:30
  29. Dmitry Karlovets (ITMO University)
    17/11/2026, 17:00
  30. Aiqiang GUO (Institute of modern physics, Chinese Academy of Sciences)
    17/11/2026, 17:30
  31. 毅程 冯 (华中师范大学)
    18/11/2026, 09:00
  32. Shuai Liu (Hunan University)
    18/11/2026, 09:00
  33. Fabio Braghin (F)
    18/11/2026, 09:20
  34. 文博 董 (University of Science and Technology of China)
    18/11/2026, 09:25
  35. 帅 王 (复旦大学)
    18/11/2026, 09:40
  36. 衷华 张 (Fudan University)
    18/11/2026, 09:45
  37. Zhe Fang (Department of Physics, Zhejiang University)
    18/11/2026, 10:00
  38. yu peiwei (Sun Yat-sen University)
    18/11/2026, 10:05
  39. Georgy Prokhorov (Joint Institute for Nuclear Research)
    18/11/2026, 10:55
  40. Dr David Wagner
    18/11/2026, 10:55
  41. 涛亚 高 (Shandong University)
    18/11/2026, 11:15
  42. Artem Roenko (Joint Institute for Nuclear Research)
    18/11/2026, 11:15
  43. Shuo Fang (中国科学技术大学)
    18/11/2026, 11:35
  44. Sota Hanai (Academia Sinica)
    18/11/2026, 11:35
  45. 宇浩 梁 (中山大学)
    18/11/2026, 11:55
  46. Eduardo Garnacho-Velasco (Eotvos Lorand University)
    18/11/2026, 11:55
  47. Yidian Chen (Hangzhou Normal University)
    18/11/2026, 14:00
  48. 德贤 韦 (Guangxi University of Science and Technology)
    18/11/2026, 14:00
  49. Mr 曈 付 (山东大学)
    18/11/2026, 14:20
  50. 梓耕 丁
    18/11/2026, 14:25
  51. Gen-Hui Li
    18/11/2026, 14:40
  52. 赵璐 欧阳 (安徽理工大学)
    18/11/2026, 14:45
  53. 轶亮 尹 (中国科学技术大学)
    18/11/2026, 15:00
  54. Hidefumi Matsuda (Fudan University)
    18/11/2026, 15:50
  55. Annamaria Chiarini (Goethe University)
    18/11/2026, 15:50
  56. 屹威 邱 (CCNU)
    18/11/2026, 16:10
  57. Andrea Vignoli
    18/11/2026, 16:10
  58. Jeremy Hansen (chinese university of Hong Kong, Shenzhen)
    18/11/2026, 16:30
  59. Zihao Liu (F)
    18/11/2026, 16:30
  60. 家荣 汪 (中国科学技术大学)
    18/11/2026, 16:50
  61. Pushpa Panday (University of Science and Technology of China)
    18/11/2026, 16:50
  62. Prof. Hong (鸿) Mao (毛) (Hangzhou Normal University)
    19/11/2026, 09:00
  63. 钰 郭 (Tsinghua University)
    19/11/2026, 09:00
  64. Mr Jin Hu (Fuzhou University)
    19/11/2026, 09:20
  65. Guangyu Zheng (University of Chinese Academy of Sciences)
    19/11/2026, 09:20
  66. Miklos Horvath (Beijing Academy of Quantum Information Sciences)
    19/11/2026, 09:40
  67. Jieke Wang (Shandong University)
    19/11/2026, 09:40
  68. José Javier Hernández Hernández
    19/11/2026, 10:00
  69. 梓谊 刘 (清华大学物理系)
    19/11/2026, 10:00
  70. Masoud Shokri (Goethe University Frankfurt)
    19/11/2026, 10:50
  71. Yaoqi Yang
    19/11/2026, 10:50
  72. Pengcheng Zhao
    19/11/2026, 11:10
  73. 栋林 王 (中国科学技术大学)
    19/11/2026, 11:10
  74. SEJAL SINGH (Sophia University, BITS Pilani)
    19/11/2026, 11:30
  75. 鑫男 朱 (Central China Normal University)
    19/11/2026, 11:30
  76. Tomoya Uji (The University of Tokyo)
    19/11/2026, 11:50
  77. Navid Abbasi
    19/11/2026, 14:00
  78. Francesco Palli (University of Florence & INFN)
    19/11/2026, 14:00
  79. Shanjin Wu (Dalian University of Technology)
    19/11/2026, 14:20
  80. yan guowei
    19/11/2026, 14:20
  81. Zhishun(志顺) Chen(陈) (Sun Yatsen University(中山大学))
    19/11/2026, 14:40
  82. Jia Ni (华中师范大学)
    19/11/2026, 14:40
  83. 硕 林 (山东大学)
    19/11/2026, 15:00
  84. Valeriya Mykhaylova (Jagiellonian University)
    19/11/2026, 15:00
  85. 翔 任 (University of Science and Technology of China)
    19/11/2026, 15:20
  86. Yi Chen (University of Science and Technology of China, China)
    19/11/2026, 15:20
  87. Wojciech Florkowski (Jagiellonian University)
    20/11/2026, 08:30
  88. Zhangbu Xu (Kent State University and Brookhaven National Lab)
    20/11/2026, 09:00
  89. Di-Lun Yang (Academia Sinica)
    20/11/2026, 09:30
  90. Prof. yi yin (chinese university of hong kong, shenzhen)
    20/11/2026, 10:30
  91. Roy Lacey (Stony Brook University)
    20/11/2026, 11:00
  92. Jinlong Zhang (Shandong University)
    20/11/2026, 11:30
  93. Kazuya Mameda (Tokyo University of Science)
    20/11/2026, 12:00
  94. 20/11/2026, 12:30
  95. Zhibin LI (Zhengzhou University), Yidian Chen (Hangzhou Normal University)
    oral

    Rotation serves as a pivotal control parameter for QCD matter, yet effective models and lattice QCD yield conflicting predictions regarding its effect on the deconfinement transition. Using a rotation-magnetic correspondence within a holographic framework, we investigate the rotational response of pure gluonic matter. Calibrated against lattice QCD data at imaginary angular velocity, we find...

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  96. Shu Lin (Sun Yat-Sen University)
    oral

    The spin correlation is believed to be a significant contribution to vector meson spin alignment. In this work, we study the generation of spin correlation through fluctuation of chromomagnetic field in the quark-gluon plasma medium. We show that anisotropic fluctuations generically lead to finite spin alignment of vector mesons. We study two sources of anisotropic chromomagnetic field...

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  97. 硕 林 (山东大学)
    oral

    Photon-induced processes in ultraperipheral collisions provide a clean probe of nuclear and particle dynamics, with azimuthal modulations offering particular sensitivity to the polarization and interaction mechanisms of quasi-real photons.Motivated by recent STAR measurements, we study azimuthal asymmetries in $\pi^+$ $\pi^-$ production near $f_2(1270)$ resonances in ultraperipheral Au+Au...

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  98. 硕 林 (山东大学)
  99. Shuo Fang (中国科学技术大学)
    oral

    We investigated the in-medium spin transport of bottomonium based on open quantum system approach with potential NRQCD interaction. We derived a Boltzmann equation describing the evolution of spin degrees of freedom and calculated the spin observables. We observe that the spin polarization of heavy quarkonium comes from its relative motion to the medium and the EE, EB, BB correlators coming...

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  100. Prof. Hong Mao (Hangzhou Normal University)
    oral

    Based on effective models (the Friedberg-Lee model, the quark-meson model, the Polyakov quark-meson model and the parity doublet model), the bubble nucleation dynamics and gravitational wave spectrum from first-order QCD phase transitions will be addressed. Our results will offer a novel probe of the origin of chiral phase transition through gravitational wave astronomy.

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  101. Georgy Prokhorov (Joint Institute for Nuclear Research)
    oral

    We show that accelerated systems exhibit a novel dissipative transport effect, driven by the gravitational trace anomaly. Unlike other famous anomalous effects, it is dissipative and manifests itself in shear viscosity, and originates from quantum entanglement across the Rindler horizon.

    To this end, we explicitly derive using Kubo formulas the shear and bulk viscosities - the entanglement...

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  102. Georgy Prokhorov (Joint Institute for Nuclear Research)
  103. José Javier Hernández Hernández
    oral

    Magnetic fields explicitly break the non-singlet flavour symmetry of QCD, since the light quarks carry unequal electric charges. The conventional mesonic partner relations used to diagnose chiral and $U(1)_A$ restoration at vanishing field must therefore be reconsidered before they can be applied at $eB \neq 0$. We show that the neutral channels retain this diagnostic role: the splitting...

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  104. 钰 郭 (Tsinghua University)
    oral

    The chiral magnetic effect (CME) provides a unique probe of anomalous chiral transport in the quark-gluon plasma, while its quantitative extraction remains challenging due to substantial background contributions and uncertainties in the underlying dynamics. In this work, we develop a data-driven framework combining event-by-event Anomalous-Viscous Fluid Dynamics (AVFD) simulations with...

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  105. Zhishun(志顺) Chen(陈) (Sun Yatsen University(中山大学))
    oral

    In relativistic heavy-ion collisions, the relative motion of heavy quarkonium with respect to the quark-gluon plasma (QGP) induces spin alignment. Our previous work attributed this to a repopulation of quarkonium's spin components, an effect rooted in the spin degree of freedom. Here we reveal a complementary mechanism, which operates at the orbital level: the relative motion between...

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  106. 梓耕 丁
    oral

    By combining Lattice QCD data with physics-informed machine learning (PIML), we investigate the behavior of the coupling constant and the quark anomalous magnetic moment (AMM) within the Nambu–Jona-Lasinio (NJL) model under a magnetic field. We train a neural network using Lattice QCD data and the analytical expression of the thermodynamic potential in the NJL model as core constraints. This...

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  107. SEJAL SINGH (Sophia University, BITS Pilani)
    oral

    The observation of global polarization of $\Lambda$ hyperons in relativistic heavy-ion collisions has motivated the development of various theoretical frameworks to describe spin polarization in strongly interacting matter. One such framework is spin hydrodynamics, in which spin degrees of freedom are incorporated as hydrodynamic variables, thereby allowing the dynamics of angular momentum to...

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  108. Shanjin Wu (Dalian University of Technology)
    oral

    Exploring the QCD phase transition is one of the most important goals in relativistic heavy-ion collisions. The Beam Energy Scan Program at RHIC has revealed a preliminary non-monotonic behavior of net-proton multiplicity fluctuations with increasing collision energy [1], which is consistent with theoretical predictions [2].

    However, the quark-gluon plasma created in relativistic heavy-ion...

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  109. Fumio Terazaki (Zhejiang Institute of Modern Physics, Department of Physics, Zhejiang University)
    oral

    Magnetic-field effects have been extensively studied in a variety of contexts, including their influence on the dynamics of heavy-ion collisions and the stabilization of certain inhomogeneous phases against thermal fluctuations. This motivates us to ask how magnetic fields affect the moat regime, which has recently attracted increasing attention as a precursor to inhomogeneous phases because...

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  110. Fumio Terazaki (Zhejiang Institute of Modern Physics, Department of Physics, Zhejiang University)
  111. Jeremy Hansen (chinese university of Hong Kong, Shenzhen)
    oral

    We investigate spin hydrodynamic properties with an focus on entropy production for massive spin 1/2 particles. We consider particle collisions both with and without the influence of chiral anomalies such as the chiral magnetic or vortical effects, encoded by Berry curvature. This manifests as a spatial shift ($\Delta$). In doing so we first define and entropy that makes use of the matrix...

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  112. Valeriya Mykhaylova (Jagiellonian University)
    oral

    We generalize the Wigner-function description of a relativistic gas of massive particles in local equilibrium to Fermi-Dirac statistics for spin-1/2 [1] and Bose-Einstein statistics for spin-1 [2]. We derive the corresponding thermodynamic currents and show that, up to second order in polarization, the resulting energy-momentum and spin tensors agree with those obtained for Boltzmann...

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  113. Valeriya Mykhaylova (Jagiellonian University)
  114. 聪 易 (华中师范大学)
    oral

    Significant global polarization of $\Lambda$ hyperons along the direction of the orbital angular momentum has been measured in non-central heavy-ion collisions where the equation of state (EOS) of the produced dense matter is expected to change from intermediate to low colliding energies. We study the sensitivity of the global $\Lambda$ polarization to EOS in heavy-ion collisions within the...

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  115. Tong Fu (Shandong University)
    oral

    The observation of hyperon polarization in heavy-ion collisions has established spin phenomena as powerful probes of QGP properties and strongly interacting matter dynamics, with global polarization directly reflecting the medium’s overall vorticity. In this talk, we present recent STAR results on the global polarization of $\Lambda$, $\Xi$, and $\Omega$ hyperons in Au+Au collisions at...

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  116. 家荣 汪 (中国科学技术大学)
    oral

    The shear-induced polarization plays a crucial role in understanding the local polarization of Λ and Λ⎯ hyperons. A key puzzle is whether the shear-induced polarization is non-dissipative or not. In this work, we analyzed the shear-induced polarization and the anomalous Hall effects using the entropy flow and H-theorem introduced from quantum (chiral) kinetic theory. While the shear-induced...

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  117. Yicheng Feng (Central China Normal University)
    oral

    Charge separation along the magnetic field as expected from the chiral magnetic effect (CME) has been studied in Au+Au collisions at $\sqrt{s_{\text{NN}}} = 200$ GeV at the Relativistic Heavy Ion Collider.
    It is quantified by the charge- and reaction plane (RP)-dependent azimuthal correlator $\Delta\gamma$.
    The elliptic-flow-induced background is removed from the measurements by comparing...

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  118. Jia Ni (华中师范大学)
    oral

    Strong magnetic fields produced in relativistic heavy-ion collisions can modify conserved-charge fluctuations and their associated chemical potentials. The Ru and Zr isobars share the same mass number, $A=96$, but have different charge-to-baryon ratios, making Ru+Ru and Zr+Zr collisions a controlled setting for isolating isospin effects. In this talk, we will present first-principles,...

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  119. Mr Zhe Fang (Department of physics, Zhejiang University)
    oral

    We investigate a rotating quantum system subjected to a co-aligned external magnetic field. The gauge-invariant kinetic angular momentum is of particular importance because as the thermodynamic conjugate of the angular velocity, it determines the equilibrium state. Its relevance is further motivated by experimental observations of extreme fluid vorticity in heavy-ion collisions. We develop a...

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  120. 翔 任 (University of Science and Technology of China)
  121. 屹威 邱 (CCNU)
    oral

    In this work, we construct a theoretical framework for relativistic second-order magnetohydrodynamics based on entropy current analysis. The formalism consistently incorporates the relaxation dynamics of dissipative fluxes, ensuring the hyperbolic nature of the evolution equations. Utilizing linear mode analysis, we investigate the constraints imposed by causality and stability on this...

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  122. Miklos Horvath (Beijing Academy of Quantum Information Sciences)
    oral

    In this talk we introduce magnetic topological insulators as a condensed-matter laboratory for exploring extensions of axion electrodynamics beyond its conventional relativistic formulation. The low-energy electronic structure of these systems is described by massive Dirac fermions coupled to electromagnetic and other symmetry-breaking background fields, providing a direct field-theoretic...

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  123. Jieke Wang (Shandong University)
    oral

    Spin correlations between hyperons provide a novel probe of spin-dependent particle production and hadronization in quantum chromodynamics (QCD). Using the high-statistics data collected by the CMS experiment, we present the first measurements of spin correlations for $\Lambda\Lambda$, $\Lambda\bar{\Lambda}$, and $\bar{\Lambda}\bar{\Lambda}$ pairs in pp collisions at $\sqrt{s}=13$ TeV and pPb...

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  124. 涛亚 高 (Shandong University)
    oral

    The spin correlation of hyperon pairs offers valuable information on the spin-spin correlation of quark-antiquark pairs generated in QCD. The first evidence of spin correlation of $\Lambda$-$\overline{\Lambda}$ pairs at short range was observed by STAR in $p+p$ collisions recently. Extending these studies to $\Lambda$-(anti)$\Lambda$ pairs produced inside jets enables a cleaner environment to...

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  125. Fabio Braghin (Federal University of Goias, Brazil)
    oral

    Some effects of weak magnetic fields on meson and constituent quark interactions and dynamics are presented at the one loop level within the Weinberg's large Nc effective field theory, and extensions, by considering a dynamical approach. The magnetic field corrections to coupling constants are found to have linear or quadratic dependence on the magnetic field, i.e. $(eB)^n$ for $n=1,2$....

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  126. Dr Daniele Roselli (University of Florence & CUHK, Shenzhen)
    oral

    We present an ab initio computation of the full nonequilibrium correction to the Wigner function of a generally interacting scalar field at freeze-out, assuming an initial state in local thermodynamic equilibrium within the framework of quantum statistical mechanics. In the hydrodynamic regime, we identify a previously overlooked dissipative memory term, proportional to the difference between...

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  127. Eduardo Garnacho-Velasco (Eotvos Lorand University)
    oral

    The study of the effect of rotation in strongly-interacting matter has drawn a lot of attention in the theoretical community, due to its relevance for heavy-ion collision experiments. Lattice simulations in the presence of rotation are commonly carried out by changing to a corotating frame, which amounts to modifying the metric. As a preparation for simulating QCD using this formalism, we...

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  128. 梓谊 刘 (清华大学物理系)
    oral

    The chiral magnetic effect (CME) in relativistic heavy-ion collisions induces a charge separation along the magnetic field, yet its detection is obscured by large backgrounds, especially from local charge conservation (LCC). Using event-by-event AVFD simulations of Au+Au collisions at $\sqrt{s_{NN}}=200$ GeV, we studied machine-learning strategies to enhance CME discrimination.
    First, we...

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  129. 梓谊 刘 (清华大学物理系)
  130. 梓谊 刘 (清华大学物理系)
  131. Eduardo Garnacho-Velasco (Eotvos Lorand University)
    oral

    We present a study of the out-of-equilibrium properties of the Chiral Magnetic Effect (CME) and the Chiral Separation Effect (CSE), both from the perturbation theory and lattice QCD perspectives. We discuss the analytic result of the retarded correlators and spectral functions of these effects at 1-loop in perturbation theory, generalizing the calculation to finite spatial momentum. The...

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  132. Andrea Vignoli
    oral

    We present the calculation of the irreducible components of the spin polarization of massive spin-3/2 particles emitted by a decoupling relativistic fluid at local thermodynamic equilibrium [A. Vignoli, F. Becattini, in preparation]. The local equilibrium calculation is performed within the framework of quantum statistical field theory using linear response theory at first order in the...

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  133. Guangyu Zheng (University of Chinese Academy of Sciences)
    oral

    Differential hyperon spin correlations may provide a new window into local chiral dynamics in relativistic heavy-ion collisions. In this talk, we study ΛΛ̄ spin correlations in Au+Au collisions at √sₙₙ = 200 GeV using AMPT supplemented with a chiral anomaly transport (CAT) module. The framework incorporates hyperon polarization induced by thermal vorticity, shear effects, and a finite axial...

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  134. 金玉 胡 (中国科学技术大学)
    oral

    Relativistic 16O+16O collisions provide a valuable opportunity to study both the quark-gluon plasma formed in small systems and the intrinsic structure of 16O. Recent implementations of ab initio nuclear configurations in heavy-ion simulations have produced different predictions for cluster-sensitive observables, making it difficult to identify the origin of possible 𝛼-cluster signals. In this...

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  135. Qiye Shou (Fudan University)
    oral

    In this talk, recent ALICE results on chirality- and vorticity-related phenomena at the LHC will be presented. New developments in the searches for the Chiral Magnetic Effect and Chiral Vortical Effect, including improved constraints and new understanding on background contributions, will be discussed. Recent measurements of global and local polarization with Run 3 data will also be highlighted.

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  136. Ankit kumar Panda (Central china normal university)
    oral

    In this work, we explore a Bemfica--Disconzi--Noronha--Kovtun (BDNK)-type formulation of relativistic magnetohydrodynamics, providing a causal and stable first-order description of dissipative fluids. We derive coupled evolution equations for the temperature and magnetic field in a boost-invariant Bjorken background, restricting to $(0+1)$D dynamics while retaining all relevant first-order...

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  137. Ankit kumar Panda (Niser)
  138. Dr Yi Chen (Tsinghua University, China)
    oral

    Spin or internal angular momentum (AM) is a fundamental property of a particle (or a generic system), and is of quantum nature. As is known to all, spin is closely related to both quantum statistics for particle distributions (e.g. the Fermi-Dirac distributions for fermions) and the Pauli exclusion principle, laying down the basic foundation for atomic structures and the evolution of the...

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  139. Yi Chen (University of Science and Technology of China, China)
  140. 帅 王 (复旦大学)
    oral

    Chiral matter exhibits a variety of intriguing anomalous transport phenomena that originate from the chiral anomaly. Prominent examples of such phenomena include the chiral magnetic effect and the chiral vortical effect. In the hydrodynamic regime, we demonstrate that in a chiral plasma subject to an external magnetic field, the chiral vortical effect can induce a new type of...

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  141. Yaoqi Yang
    oral

    Vortex states of photons, electrons, and other particles are wave packets that carry intrinsic orbital angular momentum (OAM) and exhibit other features unavailable for plane waves. Collisions of high-energy vortex states can become a promising tool for nuclear and particle physics, once experimental challenges are overcome. An extensive literature exists on scattering processes involving...

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  142. Dr Pushpa Panday (University of Science and Technology of China)
    oral

    During non-central ultra-relativistic heavy-ion collisions, the colliding nuclei carry a large global angular momentum. A part of this angular momentum is believed to be transferred to the quark-gluon plasma (QGP) medium leading to the spin polarization/alignment of the final state particles such as $\Lambda, K^{*}, \phi$. While the spin polarization of $\Lambda$ hyperons along global angular...

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  143. Peiwei Yu (Sun Yat-sen University)
    oral

    In a quark-gluon plasma, the enormous total angular momentum generated by non-central collisions evolves over time through spin-orbit coupling interactions, eventually converting into the spin component and thereby inducing spin polarization of the particles.
    Our work studies the contribution of the shear flow generated by non-equilibrium medium to the spin alignment of the vector meson J/ψ...

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  144. Artem Roenko (Joint Institute for Nuclear Research)
    oral

    Quark-gluon plasma created in heavy-ion collision experiments is affected by relativistic rotation and strong acceleration, which influence its properties. In this report, we present a lattice study of the confinement-deconfinement phase transition in rotating and accelerating gluodynamics. We find that under the influence of these extreme conditions, the finite-temperature...

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  145. Mr Wen-Bo Dong (University of Science and Technology of China)
    oral

    We propose that the anisotropic particle distributions in heavy ion collisions can induce a non-vanishing spin alignment of vector meson. We investigate this effect in the production processes of $\phi$ and $K^{*0}$ mesons. For both $\phi$ and $K^{*0}$ produced via S wave scattering, a negative $\delta\rho_{00}$ of order $10^{-3}$ is observed, whose absolute value increases in a more...

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  146. Sota Hanai (Academia Sinica)
    oral

    The Faraday effect, the rotation of the polarization plane of electromagnetic waves in a magnetized medium, is a fundamental magneto-optical phenomenon that appears across a wide range of fields, including condensed matter physics, plasma physics, and astrophysics. Although the conventional Faraday effect originates from the cyclotron motion of charged particles in a medium, the spin of the...

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  147. 德贤 韦 (Guangxi University of Science and Technology)
    oral

    Spin polarization, as a novel method for detecting the rotational properties of QGP which are produced in relativistic heavy-ion collisions, has attractd great interest. We study the impact of parton spin polarization on the effective transport and thermodynamic coefficients and the QCD critical point in non central light- and heavy-ion collisions. By employing the novel kinetic theory method,...

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  148. Francesco Palli (University of Florence & INFN)
    oral

    The polarization of Λ hyperons provides a sensitive probe of the space-time structure of the quark-gluon plasma, and in particular of the gradients of the hydrodynamic fields. Longitudinal polarization is especially sensitive to the interplay between vorticity, shear, and transport properties such as the bulk viscosity. In this talk, we review a model based on (3+1)D average event viscous...

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  149. Dr David Wagner
    oral

    We present a framework for spin dynamics in the quark-gluon plasma produced in relativistic heavy-ion collisions.

    Under the approximation of small polarization, macroscopic spin degrees of freedom decouple from the background, and their evolution equations and transport coefficients have been computed using quantum kinetic theory as an effective microscopic foundation. The resulting...

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  150. yan guowei
    oral

    The spin alignment of mesons  has been a popular subject in relativistic heavy-ion collisions . It is only until last year that non-vanishing spin alignment of  $D^{*+}$ meson was measured. We propose that through the QCD analogue of the Sokolov-Ternov effect, magnetic synchrotron radiation of gluons can polarize the $c$ and $\bar d$ quarks and result in spin alignment of $D^{*+}$ mesons. The...

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  151. Hidefumi Matsuda (Fudan University)
    oral

    We apply physics-informed neural networks (PINNs) to fully nonlinear relativistic spin hydrodynamics and study the dynamical conversion between spin and orbital angular momentum driven by the rotational viscosity, a dissipative effect intrinsic to spin hydrodynamics [1]. Such conversion is relevant to the phenomenology of relativistic heavy-ion collisions but has not been studied numerically...

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  152. Prof. xinyang wang (Anhui University of Science & Technology)
  153. Mr Yi-Liang Yin (University of Science and Technology of China)
    oral

    The spin polarization of the Lambda hyperon in low-energy Au-Au collisions can be generated by nonlocal nucleon-nucleon scattering. We introduce a wave packet for the incoming nucleons to describe the nonlocal collision. Using the chiral perturbation theory, We calculate the spin-dependent cross section with the approximations that the width of the wave packet is small and the collision energy...

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  154. Tomoya Uji (The University of Tokyo)
    oral

    In this talk, I will show that a polarized nucleon generically carries a spin-aligned dipole distribution of QCD topological charge, despite having zero total topological charge. This structure follows model-independently from the symmetry properties of the local topological charge density. Through the anomalous flavor-singlet axial Ward identity, its dipole strength is directly related to the...

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  155. Tomoya Uji (The University of Tokyo)
  156. 鑫男 朱 (Central China Normal University)
    oral

    We investigate the $U(1)_{A}$ symmetry and the chiral separation effect (CSE) in the presence of a strong background magnetic field within the three-flavor Nambu-Jona-Lasinio (NJL) model. To incorporate the inverse magnetic catalysis (IMC) effect, we introduce a magnetic-field-dependent scalar coupling $G_{s}(eB)$. We evaluate the susceptibility splittings $\chi_{\pi_{0}}-\chi_{\delta_{0}}$...

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  157. Diyu Shen (Fudan University)
  158. Prof. Igor Ivanov (SYSU, School of Physics and Astronomy)
    oral

    When describing particle collisions, we usually approximate the initial-state particles as plane waves. The fact that in reality they are wave packets does not usually play any role. However, the past two decades witnessed the emergence of a new intriguing class of wave packets called vortex states. A photon, an electron, or any other particle prepared in a vortex state is characterized by...

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