PaperPanorama

Nuclear Theory·nucl-th

Tuesday·March 25, 2025

13 papers6 primary·7 cross-listed

  1. 07

    Chiral Vortical Instability

    Shuai Wang🇨🇳 · Koichi Hattori🇨🇳 · Xu-Guang Huang🇨🇳 · Andrey V. Sadofyev🇵🇹

    We revisit the collective modes of chiral matter described by the second-order chiral hydrodynamics, noticing that chiral shear waves (CSWs) may become unstable for momenta above a characteristic scale. In the absence of sufficient dissipation, this instability emerges within the hydrodynamic regime, depending on the interplay between shear viscosity and the anomalous vortical contribution to the stress-energy tensor at second order in hydrodynamic expansion. We show that this instability generates helical flows and name it the {\it chiral vortical instability} (CVI). Alongside the chiral plasma and magnetovortical instabilities, CVI tends to transfer initial microscopic chirality into macroscopic helicities, which combine into a generalized axial charge. We further find that an elementary static Gromeka-Arnold-Beltrami-Childress flow, corresponding to a CSW at a specific momentum, solves the full nonlinear equations of second-order chiral hydrodynamics, whereas global rotation of a chiral medium is not a solution. This observation supports the relevance of CVI beyond the hydrodynamic regime. Finally, we briefly note that CVI may have multiple phenomenological implications across various systems, including QCD matter produced in heavy-ion collisions and primordial plasma in the early Universe.

    hep-thhep-phnucl-th3 citations
  2. 08

    Correlation studies of the He excited states

    M. Khirk (1, 2 and 3) · L.V. Grigorenko (1, 4 and 5) · E.Yu. Nikolskii (5 and 1) · P.G. Sharov (1 and 6) ((1) Flerov Laboratory of Nuclear Reactions, JINR, Dubna, (2) M.V. Lomonosov Moscow State University, Skobeltsyn Institute of Nuclear Physics, Moscow, (3) MIREA - Russian Technological University, Moscow, (4) National Research Nuclear University "MEPhI'', Moscow, (5) National Research Centre "Kurchatov Institute'', Moscow, (6) Institute of Physics, Silesian University in Opava, Opava)

    The unbound nucleus He was recently studied in the H(He,H)He reaction at 29 MeV beam energy in Ref.[M.S. Golovkov et al., Phys. Rev. C 109, L061602 (2024)]. The excitation spectrum of He was measured up to MeV ( is energy above the He- threshold). Angular distribution for the He- decay of the He ground state can be explained by a strong spin alignment induced by a reaction mechanism. The correlation information for the higher-lying He excitations is available as backward-forward asymmetry for the He- decay in the He frame. The asymmetry function has an expressed energy profile which may be explained by using quite restrictive assumptions about structure of He excitations or/and peculiarities of the reaction mechanism. In the analysis of [M.S. Golovkov et al., Phys. Rev. C 109, L061602 (2024)] the observation the state in He is declared with MeV. Our work is based on the same He data. However, the data analysis was improved and also the data interpretation is substantiated with the detailed PWBA reaction studies and coupled-channel calculations of the He continuous spectrum. The idea of the resonant state with is rejected. In addition, the position of the state in He is confined to the interval MeV, with ``preferred'' value 2.6 MeV. There is indication on the second state in the data with MeV and with the lower resonance energy limit MeV. Importance and prospects of more detailed correlation studies of He continuum are discussed.

    nucl-exnucl-th0 citations
  3. 09

    Search for doubly charmed dibaryons in baryon-baryon scattering

    Yao Cui🇨🇳 · Yuheng Wu🇨🇳 · Xinmei Zhu🇨🇳 · Hongxia Huang🇨🇳 · Jialin Ping🇨🇳

    We perform a systematical investigation of the doubly charmed dibaryon system with quantum numbers , and strangeness numbers , and in the framework of the chiral quark model. Two resonance states with strangeness numbers is obtained in the scattering channel, which are with resonance mass 5081 MeV and decay width 0.3 MeV, and the state with the mass 5213 MeV and decay width 19.8 MeV, respectively. These two predicted charmed dibaryon candidates are worth searching for experimentally. Besides, we would like to emphasize that the multi-channel coupling calculation is important to confirm the existence of multiquark states. The coupling can shift the energy of the resonance, give the width to the resonance and even destroy the resonance. Therefore, to provide the necessary information for experiments to search for exotic hadron states, the coupling calculation between the bound channels and open channels is indispensable.

    hep-phhep-exhep-latnucl-thPRD(2025)·2 citations
  4. 10

    Second order fluctuations of conserved charges in external magnetic fields

    Heng-Tong Ding🇨🇳 · Jin-Biao Gu🇨🇳 · Arpith Kumar🇨🇳 · Sheng-Tai Li🇨🇳

    We present a first-principles lattice QCD investigation of second-order fluctuations of and correlations among conserved charges -- baryon number (B), electric charge (Q), and strangeness (S) -- in the presence of external magnetic fields. Our study employs lattice simulations of (2+1)-flavor QCD with physical pion masses using highly improved staggered fermions (HISQ) on and lattices, covering a wide range of magnetic field strengths up to GeV. We identify clear signals of magnetic field-induced modifications to these fluctuations and correlations, with the baryon-electric charge correlation, , exhibiting particularly strong sensitivity to the magnetic field. To bridge theoretical predictions with experimental observables, we implement systematic kinematic cuts that emulate detector acceptances of the STAR and ALICE experiments within the hadron resonance gas (HRG) model and construct proxy observables for fluctuations measurable in heavy-ion collision experiments. Our findings highlight as a promising ``magnetometer" for probing the presence of magnetic fields in QCD matter. Furthermore, we explore experimentally relevant ratios involving , demonstrating their potential in mitigating volume effects and enhancing sensitivity to magnetic fields in collision environments. Additionally, we assess the limitations of the HRG model at strong magnetic fields, revealing deviations that indicate nontrivial modifications to hadronic degrees of freedom. These results offer new insights into the interplay between thermal and magnetic effects in the QCD phase diagram and provide experimentally relevant guidance for the detection of magnetic fields in heavy-ion collisions.

    hep-lathep-phnucl-exnucl-thPRD(2025)·20 citations
  5. 11

    Femtoscopy correlation functions and hadron-hadron scattering amplitudes in presence of Coulomb potential

    M. Albaladejo🇪🇸 · A. Garcia-Lorenzo🇪🇸 · J. Nieves🇪🇸

    This work addresses the incorporation of Coulomb interactions into femtoscopy correlation functions (CFs) used to probe hadron interactions. Combining strong contact potentials with Coulomb effects, the derived scattering amplitudes and wave functions are used to compute CFs, accounting for both interactions coherently. Next, we analyze the nature of the corrections due to the finite range of the strong interaction, closely linked to off-shell effects, and propose an approximate method to account for them. We show how these corrections turn out to be essential to accurately extract the strong hadron-hadron scattering amplitudes from CF data. We compare the obtained expressions for the CFs with those reported in previous theoretical frameworks. Also, using proton-proton systems as a case study, we obtain a good comparison of our results with previous realistic theoretical calculations and with accurate recent data from the ALICE experiment. The framework enables precise CF calculations without numerical solution of the Schrödinger equation, offering a practical tool for femtoscopy analyses involving charged hadrons. In addition, the scheme allows for an easy connection with scattering amplitudes obtained from Effective Field Theories.

    hep-phnucl-thPTEP(2025)·9 citations
  6. 12

    Nonperturbative Formulation of Resonances in Quantum Mechanics Based on Exact WKB Method

    Okuto Morikawa🇯🇵 · Shoya Ogawa🇯🇵

    We study quasi-stationary states in quantum mechanics using the exact Wentzel--Kramers--Brillouin (WKB) analysis as a nonperturbative framework. Whereas previous works focused mainly on stable systems, we explore unstable states such as resonances. As a concrete example, we analyze the inverted Rosen--Morse potential, which exhibits barrier resonance. This model allows exact solutions, enabling a direct comparison with exact WKB predictions. We provide a simple analytic picture of resonance and demonstrate consistency between exact and WKB-based results, extending the applicability of exact WKB analysis to nonpolynomial potentials.

    hep-thnucl-thquant-phPTEP(2025)·8 citations
  7. 13

    Gravitational form factor of the kaon in holographic QCD

    Zhibo Liu🇨🇳 · Akira Watanabe🇨🇳

    The gravitational form factor (GFF) of the kaon is investigated in a bottom-up holographic QCD model, in which the strange quark mass breaks the SU(3) flavor symmetry. The probe energy () dependence of the kaon GFF is explicitly shown and compared to that of the pion. It is presented that our result shows the behavior in the high energy region, which is consistent with the perturbative QCD prediction. The gravitational radius of the kaon is also calculated, and it is found that the result is quite close to that of the pion but slightly smaller.

    hep-phnucl-thPRD(2025)·9 citations

Affiliations

first authorsco-authorsvia INSPIRE