PaperPanorama

Nuclear Theory·nucl-th

Thursday·April 4, 2024

10 papers4 primary·6 cross-listed

  1. 01

    Learning nuclear cross sections across the chart of nuclides with graph neural networks

    Hongjun Choi · Sinjini Mitra · Jason Brodksy · Ruben Glatt · Erika Holmbeck · Shusen Liu · Nicolas Schunck · Andre Sieverding · Kyle Wendt

    In this work, we explore the use of deep learning techniques to learn how nuclear cross sections change as we add or remove protons and neutrons. As a proof of principle, we focus on the neutron-induced reactions in the fast energy regime. Our approach follows a two-stage learning framework. First, we apply representation learning to encode cross section data into a latent space using either variational autoencoders (VAEs) or implicit neural representations (INRs). Then, we train graph neural networks (GNNs) on the resulting embeddings to predict missing values across the nuclear chart by leveraging the topological structure of neighboring isotopes. We demonstrate accurate cross section predictions within a 9x9 block of missing nuclei. We also find that the optimal GNN training strategy depends on the type of latent representation used, with VAE embeddings performing best under end-to-end optimization in the original space, while INR embeddings achieve better results when the GNN is trained only in the latent space. Furthermore, using clustering algorithms, we map groups of latent vectors into regions of the nuclear chart and show that VAEs and INRs can discover some of the neutron magic numbers. These findings suggest that deep-learning models based on the representation encoding of cross sections combined with graph neural networks holds significant potential in augmenting nuclear theory models, e.g., by providing reliable estimates of covariances of cross sections, including cross-material covariances.

    nucl-thPRC(2025)·4 citations
  2. 02

    An implementation of nuclear many-body wave functions by the superposition of localized Gaussians

    Masaaki Kimura · Yasutaka Taniguchi

    We introduce a new framework for the low-energy nuclear structure calculations, which describes the single-particle wave function as a superposition of localized Gaussians. It is a hybrid of the Hartree-Fock and antisymmetrized molecular dynamics models. In the numerical calculations of oxygen, calcium isotopes and 100Sn, the framework shows its potential by significantly improving upon AMD and yielding the results consistent with or even better than Hartree-Fock(-Bogoliubov) calculations based on harmonic oscillator expansions. In addition to the basic equations, general form of the matrix elements is also given.

    nucl-thnucl-exPTEP(2024)·3 citations
  3. 03

    Softening of the Hypertriton Transverse Momentum Spectrum in Heavy-Ion Collisions

    Dai-Neng Liu🇨🇳 · Che Ming Ko🇺🇸 · Yu-Gang Ma🇨🇳 · Francesco Mazzaschi🇮🇹 · Maximiliano Puccio🇨🇭 · Qi-Ye Shou🇨🇳 · Kai-Jia Sun🇨🇳 · Yuan-Zhe Wang🇨🇳

    Understanding the properties of hypernuclei helps to constrain the interaction between hyperon and nucleon, which is known to play an essential role in determining the properties of neutron stars. Experimental measurements have suggested that the hypertriton (), the lightest hypernucleus, exhibits a halo structure with a deuteron core encircled by a hyperon at a distance of about 10 fm. This large distance in wave function is found to cause a suppressed yield and a softening of its transverse momentum () spectrum in relativistic heavy-ion collisions. Within the coalescence model based on nucleons and hyperons from a microscopic hybrid hydro model with a hadronic afterburner for nuclear cluster production in Pb-Pb collisions at = 5.02 TeV, we show how this softening of the hypertriton spectrum appears and leads to a smaller mean for than for helium-3 (He). The latter is opposite to the predictions from the blast-wave model which assumes that and He are thermally produced at the kinetic freeze-out of heavy-ion collisions. The discovered quantum mechanical softening of the (anti-)hypertriton spectrum can be experimentally tested in relativistic heavy-ion collisions at different collision energies and centralities and used to obtain valuable insights into the mechanisms for light (hyper-)nuclei production in these collisions.

    nucl-thhep-phPLB(2024)·23 citations
  4. 04

    Spin alignment of induced by strange-baryon density inhomogeneity

    Feng Li🇨🇳

    The difference between the spin alignments of and those of at the low collision energies is a puzzle raised by the recent experiments. Unlike meson, , carrying a unit strange charge, should react to strange chemical potential . In this paper, we shall first convince you that is not small in a brayon-rich medium for keeping strange neutrality, and then derive the spin alignment induced by the gradient of , and hence of baryon chemical potential , using linear response theory, with the transport coefficients expressed, without any approximation, in terms of the 's in-medium spectral properties by employing Ward-Takahashi identity. It turns out that such an effect applies mainly to the particles whose longitudinal and transverse modes diverge, and induces only the local spin alignment in a static medium. The magnitudes of these coefficients will be further estimated under the quasi-particle approximation.

    nucl-thhep-phPRC(2024)·5 citations
  5. 05

    Avenues for a number density interpretation of dihadron fragmentation functions

    T. Rogers🇺🇸 · A. Courtoy🇲🇽

    In this comment, we reassess the underlying physics of the number sum rule for dihadron fragmentation functions. We will argue that, currently, there are no settled constraints on what constitutes a valid number density interpretation for multihadron fragmentation functions. Imposing overly restrictive criteria might lead to misinterpretating the data. Most importantly, and on the basis of phenomenological analyses, the slightly varying definitions used in previous work are not excluded from possessing legitimate number density interpretations (up to the usual issues with ultraviolet divergences and renormalization), so long as they are paired with appropriate factorization theorems. We advocate for further theoretical analyses to be challenged with experimental data, available at JLab or at the future EIC.

    hep-phnucl-exnucl-thRev.Mex.Fis.(2025)·2 citations
  6. 06

    Net proton number cumulants from viscous hydro with equation of state including a critical end point

    Yi-fan Shen🇨🇳 · Wei Chen🇨🇳 · Xiang-yu Wu🇨🇦 · Kun Xu🇨🇳 · Mei Huang🇨🇳

    In the SMASH-CLVisc-hybrid framework, including SMASH for the initial conditions and the hadronic rescattering stage, and CLVisc for the quark gluon plasma (QGP) evolution, we investigate net baryon number fluctuations via considering the equation of state (EoS) with and without a critical end point (CEP) in the QCD phase transition. Specifically, two distinct QCD EoS are utilized: one with smooth crossover derived from NEOS and another with a critical end point sourced from the rPNJL model. Our results show that non-monotonic behavior of is not observed above the collision energy , nor are there explicit differences between the EoS characterized by crossover and that by CEP. This could be attributed to the significant deviation of the freeze-out line from the location of CEP. It is also found that the pure SMASH result of is positive and close to zero at 3 GeV, which is different from the negative value observed from STAR.

    hep-phnucl-thPRC(2025)·3 citations
  7. 07

    Universality of Efimov states in highly mass-imbalanced cold-atom mixtures with van der Waals and dipole interactions

    Kazuki Oi · Pascal Naidon · Shimpei Endo

    We study three-body systems in a mass-imbalanced two-component cold-atom mixture, and we investigate the three-body parameter of their Efimov states for both bosonic and fermionic systems, with a major focus on the Er-Er-Li Efimov states. For a system interacting solely via van der Waals interactions, the van der Waals universality of the three-body parameter is analytically derived using the quantum defect theory. With the addition of a perturbative dipole interaction between the heavy atoms, the three-body parameters of the bosonic and fermionic Efimov states are found to behave differently. When the dipole interaction is as strong as the van der Waals interaction, corresponding to realistic Er-Er-Li Efimov states, we show that the van der Waals universality persists once the effects of the non-perturbative dipole interaction are renormalized into the s-wave and p-wave scattering parameters between the heavy atoms. For a dipole interaction much stronger than the van der Waals interaction, we find that the universality of the Efimov states can be alternatively characterized by a quasi-one-dimensional scattering parameter due to a strong anisotropic deformation of the Efimov wavefunctions. Our work thus clarifies the interplay of isotropic and anisotropic forces in the universality of the Efimov states. Based on the renormalized van der Waals universality, the three-body parameter is estimated for specific isotopes of Er-Li cold-atom mixtures.

    cond-mat.quant-gasnucl-thPRA(2024)·6 citations
  8. 08

    Deep learning for flow observables in high energy heavy-ion collisions

    H. Hirvonen🇫🇮 · K.J. Eskola🇫🇮 · H. Niemi🇫🇮

    We demonstrate how deep convolutional neural networks can be trained to predict 2+1 D hydrodynamic simulation results for flow coefficients, mean-transverse-momentum and charged particle multiplicity from the initial energy density profile. We show that this method provides results that are accurate enough, so that one can use neural networks to reliably estimate multi-particle flow correlators. Additionally, we train networks that can take any model parameter as an additional input and demonstrate with a few examples that the accuracy remains good. The usage of neural networks can reduce the computation time needed in performing Bayesian analyses with multi-particle flow correlators by many orders of magnitude.

    hep-phnucl-thEPJ Web Conf.(2024)·3 citations
  9. 09

    Light-quark mass dependence of the resonance

    Xiu-Lei Ren🇩🇪

    We present the light-quark mass dependence of the resonance at leading order in a renormalizable framework of covariant chiral effective field theory. The meson-baryon scattering amplitudes, which are obtained by solving the scattering equation within time-ordered perturbation theory, follow the quark mass trajectory of the Coordinated Lattice Simulations consortium. At MeV and MeV, our parameter-free prediction of poles is consistent with the recent lattice results of BaSc Collaboration [Phys. Rev. Lett. 132, 051901 (2024)]. Varying the pion mass from MeV to MeV, we present the evolution of double-pole positions of : the higher pole remains a resonance around the threshold; whereas the lower pole undergoes a transition from resonance to a virtual state, and ultimately to a bound state of the system, which could be verified by the forthcoming lattice QCD simulations.

    hep-phnucl-thPLB(2024)·11 citations
  10. 10

    Pre-equilibrium Photon and Dilepton Production

    Oscar Garcia-Montero🇩🇪 · Aleksas Mazeliauskas🇩🇪 · Philip Plaschke🇩🇪 · Sören Schlichting🇩🇪

    We use QCD kinetic theory to compute photon and dilepton production in the chemically equilibrating out-of-equilibrium quark-gluon plasma created in the early stages of high-energy heavy-ion collisions. We derive universal scaling functions for the pre-equilibrium spectra of photons and dileptons. These scaling functions can be used to make realistic predictions for the pre-equilibrium emission and consequently establish the significance of the pre-equilibrium phase for the production of electromagnetic probes in heavy-ion collisions.

    hep-phnucl-thEPJ Web Conf.(2024)·3 citations

Affiliations

first authorsco-authorsvia INSPIRE