PaperPanorama

Nuclear Theory·nucl-th

Tuesday·August 4, 2026

23 papers15 primary·8 cross-listed

  1. 01

    Nuclear -Ray Cascades as Markov Processes

    A. Psaltis

    A framework for computing -ray feeding probabilities in nuclear decay schemes based on absorbing Markov chains is presented. In this approach, excited nuclear states are treated as transient states and long-lived levels as absorbing states, allowing feeding fractions to be obtained exactly from the transition matrix. Experimental uncertainties are propagated via Monte Carlo sampling from Dirichlet distributions, which naturally maintains the physical constraint of unit normalization for branching-ratio vectors. This framework is applied to the key keV resonance in the Mg(p,)Al reaction ( keV), which governs the production of Al in hydrogen-burning environments. Combining multiple experimental datasets within a Hierarchical Bayesian framework, a ground-state feeding probability of is found, and for the first time the dominant -decay transitions contributing to its uncertainty are identified. The formalism reproduces traditional cascade calculations while providing analytic sensitivity information and a transparent uncertainty decomposition. This approach offers a general and computationally efficient tool for propagating nuclear-structure uncertainties to astrophysical reaction rates and can be readily extended to other nuclei.

    nucl-thnucl-exPRC(2026)·0 citations
  2. 02

    Constraining tensor force terms with the charge radii difference of mirror-pair nuclei

    Yan Ya · Na Tang · Rong An

    Charge radii differences of mirror partner nuclei provide an alternative probe to pin down the interaction components in asymmetric nuclear matter. In this work, the differences in the charge radii of almost spherical mirror-paired nuclei Ni-Fe and Ca-S are used to constrain the magnitude of tensor terms in the Skyrme interactions. The calculated results suggest that a linear correlation can be found between the difference of charge radii of mirror partner nuclei and the adopted strengths of the triplet-odd and triplet-even tensor components. Besides, it suggests that charge radii differences of mirror-paired nuclei are more sensitive to the adopted strengths of the triplet-odd parameter rather than the triplet-even parameter . Combining the quantitative constraint strengths of the triplet-even tensor part obtained from the magnetic dipole (M1) excitations, the charge-exchange Gamow-Teller (GT) states, and the spin-dipole (SD) excitations, the triplet-odd strengths are further constrained for the SLy5 as well as SGII effective interactions. This provides an alternative approach to constrain the appropriate magnitude of tensor force.

    nucl-thPRC(2026)·0 citations
  3. 04

    Schrödinger Generator for High-Dimensional Integration and Sampling on Quantum Many-Body States

    Lin-Jing Jiang · Fu Ma · Pei Li · Kai-Jia Sun · Guo-Liang Ma · Yu-Gang Ma

    Integration and sampling in high dimensions are among central challenges in modern science and technology, underlying applications ranging from quantum many-body physics to Bayesian inference and artificial intelligence. Although conventional Monte Carlo methods are formally scalable, their efficiency deteriorates rapidly in the presence of strong correlations or sharp features in high-dimensional configuration space. Here we introduce a new framework, termed the Schr"odinger Generator, for integration and sampling based on the explicit optimization of coordinate transformations. The method decomposes the total Jacobian into two complementary components, including an adaptive map that minimizes estimator variance by learning the marginal structure in each dimension, and a normalizing-flow-based transformation that captures non-factorizable correlations in the target distribution. A final resampling step guarantees unbiased sampling even when the learned transformation is imperfect. We demonstrate stable and scalable performance for nuclear quantum many-body states in dimensions exceeding 600. Short-range correlations among nucleons in finite nucleus are faithfully reproduced. The framework offers a physically transparent approach to high-dimensional stochastic integration and sampling, opening new possibilities for simulations of complex quantum systems.

    nucl-thquant-ph1 citation
  4. 05

    Deformation effects on reaction observables of beryllium nuclei from ab initio densities

    Qi Lu · Rui-Feng Tian · Shi-Sheng Zhang · Ulf-G. Meißner · Shihang Shen

    We combine three-dimensional intrinsic densities from ab initio nuclear lattice effective field theory with a deformed Glauber model to study high-energy reactions of {7-12}Be. To connect the correlated many-body configurations to the core-plus-neutron reaction formalism without imposing a single-particle orbital, we introduce a configuration-resolved prescription that identifies the spatially outermost valence neutron after the two-cluster decomposition. For Be projectiles on 12C and 9Be targets at 790 MeV/A, explicit orientation averaging lowers the calculated reaction cross section of 11Be by up to approximately 50 mb relative to a calculation with the spherically averaged density. The deformed calculation reproduces the pronounced increase from 10Be to the established one-neutron halo nucleus 11Be for both targets. We further calculate the momentum distribution of the fragments after the one-neutron removal reaction of 11Be + 9Be , finding good agreement in shape with the measurement at 63 MeV/A and providing a prediction at 790 MeV/A. These results quantify how intrinsic deformation and weak binding are transmitted from microscopic many-body densities to reaction observables.

    nucl-th0 citations
  5. 06

    Proton-proton Femtoscopy as a Probe of Short-range Structure in High-Energy O+O Collisions

    Baoshan Xi🇨🇳 · Pei Li🇨🇳 · Chunjian Zhang🇨🇳 · Jinhui Chen🇨🇳 · Su-Ya-La-Tu Zhang🇨🇳 · Yu-Gang Ma🇨🇳

    Short-range nucleon-nucleon correlations are a defining feature of the nuclear many-body wave function, yet they are invisible in the one-body density and therefore inaccessible to observables that measure a nuclear size. We show that proton-proton femtoscopy supplies the missing sub-femtometer sensitivity. In O+O collisions at 200 GeV, we compare three nuclear-structure inputs spanning mean-field, low-resolution cluster, and short-range-correlated descriptions. The - correlation function separates all three, most sharply in peripheral collisions, where the \textit{ab initio} input suppresses the extracted source radius by relative to the mean-field baseline. Under identical conditions - correlations respond an order of magnitude more weakly, and the double ratio retains the full effect, pointing to the short-distance weighting of the pair rather than to an overall rescaling of the source. The signal survives the leading theoretical systematic, the choice of strong-interaction potential, which we quantify explicitly. These results identify - femtoscopy as a short-distance-resolved probe of light-nucleus structure, complementary to flow observables that constrain only the low-order moments of the initial geometry.

    nucl-thnucl-ex0 citations
  6. 07

    Multipartite entanglement study in -shell nuclei

    Rohit M. Shinde · Praveen C. Srivastava

    In this study, we present multipartite entanglement results for the Ca and Ti isotopic chains obtained from nuclear shell-model wavefunctions. Our investigation focuses on the first excited states, which exhibit signatures of shell closures at and . We calculate the 4- and 6-tangles, together with their corresponding network representations, providing a detailed picture of the underlying many-body correlations among nucleons. The primary objective of this work is to investigate the influence of shell closures on higher-order -tangles, thereby gaining insight into the evolution of multipartite entanglement in medium-mass nuclei.

    nucl-th0 citations
  7. 08

    Quantum Simulation of Nuclear Shell Model Using GCM-Based Methods on NISQ Devices

    Durgesh Pandey🇮🇳 · Ashutosh Singh🇮🇳 · Ankit Kumar Das🇮🇳 · P. Arumugam🇮🇳

    Based on the Generator Coordinate Method (GCM), we use a Quantum GCM (QuGCM) within a hybrid quantum-classical framework to simulate low-lying eigenstates of nuclear systems on quantum devices. The generator basis states are constructed from Hartree-Fock (HF) reference states, excited via symmetry-adapted unitary coupled-cluster (UCC) operators. These states are prepared as non-orthogonal quantum circuits and measured pairwise to compute the required overlap and Hamiltonian kernels. The resulting data is processed using a classical generalized-eigenvalue solver, following the GCM formalism, to extract the system's energy spectrum. To enhance efficiency and reduce circuit depth, we apply the Adaptive Generator Coordinate Inspired method (ADAPT-GCIM), which iteratively selects generator excitations based on energy gradients, thereby avoiding the need to explore the full Hilbert space. Our implementation is applied to nuclear systems, specifically the deuteron with the Reid68 potential and shell-model Hamiltonians of Li and Ar. For each system, both the QuGCM and ADAPT-GCIM methods produce energy spectra in agreement with classical diagonalization results, demonstrating robustness even under noise and limited-depth constraints. Additionally, we compare fermionic encoding strategies, specifically Jordan-Wigner (JW) transformations of one-hot (OH) encoding and Gray code (GC) mappings, and show that GC encoding reduces circuit complexity and improves fidelity during multi-reference state preparation. Our findings indicate that QuGCM and ADAPT-GCIM provide a practical and scalable path toward simulating correlated quantum systems, with lesser vulnerability to noise and better compatibility with the limitations of current quantum hardware.

    nucl-thquant-ph2 citations
  8. 09

    Necessary and sufficient conditions of nonlinear causality in viscous anisotropic hydrodynamics

    Kento Yoshida🇯🇵 · Shujun Zhao🇯🇵 · Tetsufumi Hirano🇯🇵

    We derive the necessary and sufficient conditions for nonlinear causality in viscous anisotropic hydrodynamics (VAH) within the approximation that neglects small correction terms. Relativistic hydrodynamics provides a successful description of the space-time evolution of the matter produced in relativistic heavy-ion collisions, yet the earliest stage at which a hydrodynamic description becomes valid remains an open question. VAH has been proposed as an extension of conventional viscous hydrodynamics (VH) that can accommodate the large pressure anisotropies of the early-time dynamics. However, in such far-from-equilibrium regimes, the nonlinear causality of the theory is not guaranteed. By analyzing the characteristic velocities of the VAH equations of motion, we derive a set of inequalities that ensures causal signal propagation in all directions. The resulting conditions take a remarkably simple form and admit a clear physical interpretation in terms of the characteristic modes of the anisotropic medium. These results establish the regime of validity of VAH and provide a foundation for its application to the early-time dynamics of relativistic heavy-ion collisions.

    nucl-thhep-phnucl-ex0 citations
  9. 10

    Theoretical Review of Critical Point Predictions

    Maneesha Sushama Pradeep

    This review summarizes recent theoretical progress on the QCD equation of state near the critical point and developments in the maximum entropy freeze-out framework, which provides a systematic connection between hydrodynamic fluctuations and hadronic multiplicity cumulants. We also discuss recent applications of this framework, together with advances in the dynamical evolution of critical fluctuations.

    nucl-thhep-ph0 citations
  10. 11

    Diffusion and shear viscosity coefficients of hot isospin asymmetric strange hadronic matter using a chiral SU(3) model

    Amruta Mishra · Shujun Zhao · Tetsufumi Hirano

    We study the diffusion and shear viscosity coefficients of hot isospin asymmetric strange hadronic matter. The effects due to the baryon density, isospin, strangeness, and temperature on the nucleons and hyperons are studied within a chiral SU(3) model. The medium modifications of the baryons arise due to interactions with the mean scalar and vector fields within the model. The thermodynamic and transport properties are studied in the hot strange hadronic matter. The diffusion matrix associated with the multiple charges (baryon number, isospin, and strangeness), as well as the coefficient of shear viscosity, are computed from the Boltzmann equation using first-order Chapman--Enskog expansion within the relaxation time approximation. There are observed to be significant effects from the isospin asymmetry as well as the strangeness of the medium on the diffusion coefficients. The coefficient of shear viscosity, is observed to have a large enhancement in the presence of finite strangeness in the medium due to additional contributions from the hyperons. The effects due to isospin asymmetry on the shear viscosity coefficient is however observed to be marginal both in nuclear and hyperonic matter. The present study can be relevant for the experimental observables of asymmetric relativistic heavy-ion collisions, e.g., in the compressed baryonic matter (CBM) experiment at the FAIR facility at GSI as well as in the future J-PARC-HI program.

    nucl-thhep-ph0 citations
  11. 12

    An exact time-dependent generator coordinate method with projection for spontaneous fission reactions

    N.-W. T. Lau🇫🇷 · G. Scamps🇫🇷 · P. Tan🇫🇷 · R. N. Bernard🇫🇷

    Microscopic descriptions of fission dynamics through the barrier rely on different theoretical frameworks depending on the fission regime, with the time-dependent generator coordinate method (TDGCM) commonly used for induced fission and semiclassical approaches such as the Wentzel-Kramers-Brillouin (WKB) method widely employed for spontaneous fission. In this work, we develop a fully microscopic approach to spontaneous fission based on an exact formulation of the TDGCM, avoiding both the Gaussian overlap approximation and semiclassical treatments. By combining the exact TDGCM with new projection tools and a quasistatic description of spontaneous fission, we derive spontaneous fission lifetimes from a one-dimensional potential energy surface. A detailed analysis of the model parameters shows that they do not introduce uncontrolled phenomenological effects. Remaining discrepancies with experimental lifetimes are traced to possible limitations of the underlying microscopic interaction and to the choice of basis states in the generator coordinate method. The new framework provides a microscopic description of spontaneous fission with reduced empirical input and offers a pathway toward improved predictions through future developments of nuclear interactions, collective coordinates, and the handling of many-body dynamics.

    nucl-th0 citations
  12. 13

    Probing Quadruple Deformation in Transitional Nuclei via Angular Momentum Projection

    Xian-Zhi Zhao · Sheng-Nan Wang · Yu Zhang

    Within the interacting boson model (IBM), a geometric analysis of transitional nuclei is carried out through angular momentum projection of the intrinsic coherent state. The results indicate that -mixing effects in the calculations are typically negligible, validating the use of -fixed projection for semiclassical analyses of the spin dependence of quadrupole deformation in the IBM. Further analysis indicates that in a rotating transitional system, quadrupole deformation is stretched with increasing angular momentum, providing a geometrically intuitive perspective on the commonly observed Jacobi-type transitions, as exemplified by the case studies of Gd and Dy. The method is additionally applied to the yrast states of Os to probe quadrupole deformation changes linked to the observed low-spin anomaly behavior, demonstrating the capability of IBM-based angular momentum projection in interpreting exotic collective phenomena.

    nucl-thPRC(2026)·0 citations
  13. 14

    Effects of light-cluster degrees of freedom on collective flows in heavy-ion collisions at FOPI energies

    Xin Li🇨🇳 · Si-Pei Wang🇨🇳 · Rui Wang🇨🇳 · Zhen Zhang🇨🇳 · Jie Pu🇨🇳 · Chun-Wang Ma🇨🇳 · Lie-Wen Chen🇨🇳

    Within a lattice Boltzmann-Uehling-Uhlenbeck transport model coupled to a kinetic approach for light-cluster formation, we investigate the impact of explicit light-cluster degrees of freedom on collective flows in Au+Au collisions at FOPI energies with beam energies = -- MeV by using a density-, momentum-, and isospin-dependent NLO Skyrme pseudopotential. We first benchmark the kinetic approach by comparing the calculated light-cluster yields with FOPI data in central Au+Au collisions. We then analyze the collective flows of protons and light nuclei (deuterons, tritons, , and ) in mid-central collisions. For protons, calculations with and without dynamical light-cluster degrees of freedom are compared to quantify the influence of dynamical cluster formation on proton directed (), elliptic (), triangular (), and quadrangular () flows. We find that the dynamical light-cluster effect appreciably modifies proton -- flows at -- MeV, remains visible at -- MeV, and gradually weakens at MeV. For light nuclei, the kinetic approach captures the overall beam-energy dependence of the FOPI flow data, with better agreement for MeV. We further examine the nucleon-number scaling of in both model calculations and experimental data, finding that the kinetic light-cluster formation approach qualitatively reproduces the observed scaling behavior. These results highlight the importance of a dynamical treatment of light-cluster formation for interpreting collective flows in heavy-ion collisions below about MeV, although the clustering effects on proton flows are minor at higher collision energies.

    nucl-thhep-exhep-phnucl-ex0 citations
  14. 15

    The -mode frequencies in cold neutron stars and nuclear saturation parameters

    Hajime Sotani · Hajime Togashi

    Oscillation frequencies excited in neutron stars are crucial for extracting their interior properties. In addition to the fundamental and pressure modes, the gravity (-) modes can be excited even in zero-temperature stellar models due to the composition gradient. In this study, we systematically study the -mode frequencies, focusing on the nucleonic equation of state. Then, we can derive an empirical relation for the 1st -mode frequencies as a function of the stellar compactness and the combination of the nuclear saturation parameters, , where and denote the incompressibility of symmetric nuclear matter and the density dependence of the nuclear symmetry energy, respectively. If an observed 1st -mode frequency significantly deviates from our empirical relation, it may indicate the emergence of additional degrees of freedom or new compositions inside the star.

    nucl-thastro-ph.HEPRD(2026)·0 citations
  15. 16

    Effects of equilibrium coexisting phases in the first-order chiral transition within the Linear sigma model with quarks

    R. M. Aguirre🇦🇷

    The first order chiral phase transition for quark matter with flavor imbalance is studied using the Linear sigma model with quarks, also known as Quark-meson model. Special attention is paid to the role of the scalar isovector meson. The general consensus presently is that the chiral transition changes from a smooth crossover to first-order at low temperatures. This transition is assumed to be discontinuous, with unstable or metastable intermediate states. However, if multiple charges are simultaneously conserved the system could undergo a continuous change through a coexistence of equilibrium states. Under such assumption the bulk properties are analyzed and several remarkable effects for the speed of sound and the susceptibilities are stressed.

    hep-phnucl-thPRC(2026)·0 citations
  16. 17

    Testing Lepton Wave Function Factorization in Electron Capture

    M. Cadeddu🇮🇹 · N. Cargioli🇮🇹 · M. Cau🇮🇹 · F. Dordei🇮🇹 · L. Ferro🇮🇹

    Electron-capture ratios provide precision tests of atomic wave functions and of possible non-factorization effects in nuclear electron capture. By exploiting exact leptonic wave functions, we present a general framework for predicting the electron capture rates of . Adopting a non-factorized treatment of the transition matrix element, we investigate the interplay between the nuclear transition density, which encodes the nuclear structure contribution, and the leptonic wave functions. Using phenomenologically constrained transition densities, we quantify the impact of non-factorization effects on the capture rates. Finally, we compare our theoretical predictions for the , and electron capture ratios with the current experimental world averages, providing an up-to-date assessment of the theoretical and experimental status of electron capture.

    hep-phnucl-th0 citations
  17. 18

    Misconceptions About the Physics of the QCD Trace Anomaly from Renormalization in a Reducible Basis

    Chen Yang🇺🇸

    The QCD trace anomaly is a well-established textbook result in quantum field theory with several prominent features: (1) it arises from the quantum breaking of scale symmetry at ultraviolet (UV) scales, yet is independent of the particular UV regulator used, whether lattice or dimensional regularization; (2) although it is nominally proportional to (), it is free of renormalization-scheme ambiguity; and (3) it is free of UV divergences and is therefore scale independent. Unfortunately, these important features have been undermined in the recently introduced reducible-basis renormalization, leading to misunderstandings of anomaly-related nucleon physics, including the origins of nucleon mass and internal forces.

    hep-phhep-latnucl-th0 citations
  18. 19

    Model analysis on the effectiveness of the HAL QCD method for hadron-hadron interactions

    Takayasu Sekihara🇯🇵 · Kei Fujiwara🇯🇵

    The HAL QCD method has been one of the powerful tools to extract hadron-hadron interactions directly from lattice QCD simulation data. In this paper, we aim at examining the effectiveness of the HAL QCD method by deriving a formula to calculate quantities in the HAL QCD method, such as the so-called R-correlators and HAL QCD local potentials, from the hadron-hadron scattering amplitudes within effective models. In this framework, we can judge whether the HAL QCD local potential, evaluated in the present formula, reproduces the properties of the original hadron-hadron interaction or not via the scattering amplitude, which is a solution of the Lippmann--Schwinger equation with the original hadron-hadron interaction as an input. In an analysis within a simple model of elastic scattering, we show that, when the original interaction is predominantly local, the HAL QCD local potentials quantitatively reproduce phase shifts of the hadron-hadron scatterings and correctly indicate the existence/absence of the bound state with its binding energy MeV. Lattice discretization of spacetime modifies the results only slightly. Furthermore, we consider the potential in a bare to transition amplitude, which shows singular behavior around the origin in the recent HAL QCD results of the lattice QCD simulation data, and discuss the cause of such singular behavior in the HAL QCD method through our model analysis of the scattering.

    hep-phhep-latnucl-th0 citations
  19. 20

    A femtoscopic tale of two -parities: the and the isovector partner of the

    Pan-Pan Shi🇪🇸 · Miguel Albaladejo🇪🇸 · Feng-Kun Guo🇨🇳 · Juan Nieves🇪🇸

    Understanding the nature of the exotic and states, and searching for the predicted isovector partner of the , remain central challenges in exotic-hadron spectroscopy. We investigate the femtoscopic correlation functions (CFs) of the systems. Since these charm-meson--antimeson pairs are not -parity eigenstates, their CFs contain contributions from both the -odd and -even sectors, providing direct access to the dynamics underlying the , , and the predicted isovector exotic . Within a heavy-quark-spin-symmetric coupled-channel framework, we show that the -even admixture enhances the low-momentum CFs by more than in the vicinity of their thresholds. Free from Coulomb distortions and accessible in high-multiplicity collisions at the LHC, these channels offer the first direct femtoscopic probe of the isovector -even sector and of the elusive state.

    hep-phhep-exnucl-exnucl-th0 citations
  20. 21

    Properties of the in hot and dense nuclear matter

    Tomona Kinugawa🇯🇵 · Àngels Ramos🇪🇸 · Laura Tolos🇪🇸

    We investigate the properties of the in hot and dense nuclear matter using a coupled-channel molecular model built on next-to-leading-order heavy meson chiral perturbation theory. In-medium modifications to the stem from changes to the channel within the coupled - system. As nuclear density increases, the quasiparticle peak shifts toward lower energies and broadens, tracking the behavior of the -meson spectral function. As for temperature effects, those are milder, with the thermal smearing of the Fermi surface and the melting of excitations in the -meson spectral function shifting the peak back toward its free-space mass while narrowing it. Conversely, the behavior of the is governed by the channel and its medium behavior is driven by the spectral function. With increasing temperature, the also approaches its free-space mass, but its width broadens before saturating at high temperatures. Incorporating explicit medium dependencies into the interaction kernel, driven by density and/or temperature variations in the pion decay constant, further shifts the mass lower and narrows its width with temperature. As for , its mass also drops with temperature but its width increases. These contrasting medium behaviors offer a promising pathway to constrain the internal structure of these exotic states.

    hep-phnucl-th0 citations
  21. 22

    What are the consequences of independent factorization and renormalization scales?

    T.C. Rogers🇺🇸 · R.M. Whitehill🇺🇸

    It is common for separate factorization and renormalization scales to be discussed in connection with phenomenological applications of QCD factorization theorems. We observe that simultaneously preserving renormalization group invariance, Ward identities, and the basic sum rules in the definitions of parton densities forces these scales to be equal. The statement applies to generalized pole subtraction schemes that use dimensional regularization and to collinear factorization theorems for basic processes like deep inelastic scattering. We discuss implications for estimating the effects of scale sensitivity in phenomenological calculations, consistent extractions of Standard Model parameters alongside parton densities in global QCD analyses, and generally connecting phenomenologically extracted parton densities to first principles non-perturbative techniques like lattice QCD.

    hep-phhep-thnucl-th0 citations
  22. 23

    The -dimensional Gross-Neveu-Yukawa model at finite temperature, density, and magnetic field within the Functional Renormalization Group

    Justin L.P. Mauldin🇩🇪 · Dirk H. Rischke🇩🇪

    We investigate the phase diagram of the (2+1)-dimensional Gross-Neveu-Yukawa (GNY) model at finite temperature, density, and magnetic field beyond mean-field, using the Functional Renormalization Group (FRG) in the local potential approximation. Large magnetic fields result in magnetic catalysis, a dimensional reduction of the system, and enhancement of chiral symmetry breaking. We employ a hydrodynamical algorithm to solve the FRG flow equation for the effective potential, which allows for go further into the infrared region than with previously used methods. We find that the chiral condensate exhibits non-trivial behavior in various regions of the phase diagram: several first-order phase transitions and de Haas -- van Alphen oscillations at small magnetic field and large chemical potential, as well as a critical endpoint which shifts to higher temperature with increasing magnetic field.

    hep-phhep-thnucl-th1 citation

Affiliations

first authorsco-authorsvia INSPIRE