PaperPanorama

Nuclear Theory·nucl-th

Thursday·October 10, 2024

15 papers8 primary·7 cross-listed

  1. 01

    The Hypertriton Puzzle in Relativistic Heavy-Ion Collisions

    Thomas Cohen🇺🇸 · Maneesha Pradeep🇺🇸

    The yields of hadrons and light nuclei in relativistic collisions of heavy-nuclei at a center of mass energy of 2.6 TeV can be described remarkably well by a thermal distribution of an ideal gas of hadrons and light nuclei interacting only via the decay of resonances. Given the particularly small binding energy of hypertritons relative to the temperature describing the yields (about 156 MeV), one might naturally expect hypertrions to dissociate in medium, making the agreement of hypertriton yields with thermal predictions highly puzzling. The puzzle is compounded by the fact that small binding energy is associated with the large size of the hypertriton. This size is on a similar scale to the overall size of the fireball and much larger than the length scale over which temperatures in the fireball vary over phenomenologically relevant amounts. This paper quantifies the tension this effect causes and shows that it is sufficiently large to render the thermal model inconsistent: its natural assumptions are in conflict with its outputs. The possibility that hypertritons are formed at freeze out as compact objects, quark droplets, that subsequently evolve into hypertritons is considered as a way to resolve the puzzle. It is noted that beyond making the assumption that compact quark droplets form, additional detailed dynamical assumptions which have not been justified are needed to make the thermal model work. The issue of why, despite these issues, the hypertriton is well described by a simple statistical description at freeze out is unresolved. Resolving the hypertriton puzzle is important as it may clarify whether the phenomenological success of the simple thermal model for yields accurately reflects the simple picture of the underlying physics on which it is based.

    nucl-thhep-phPRC(2025)·3 citations
  2. 02

    16O electroweak response functions from first principles

    Bijaya Acharya🇺🇸 · Joanna E. Sobczyk🇩🇪 · Sonia Bacca🇩🇪 · Gaute Hagen🇺🇸 · Weiguang Jiang🇩🇪

    We present calculations of various electroweak response functions for the 16O nucleus obtained using coupled-cluster theory in conjunction with the Lorentz integral transform method. We employ nuclear forces derived at next-to-leading order and next-to-next-to-leading order in chiral effective field theory and perform a Bayesian analysis to assess uncertainties. Our results are in good agreement with available electron-scattering data at q~ 326 MeV/c. Additionally, we provide several predictions for the weak response functions in the quasi-elastic peak region at q= 300 and 400 MeV/c, which are critical for long-baseline neutrino experiments.

    nucl-thPRL(2025)·20 citations
  3. 03

    White Dwarf Structure and Binary Inspiral Gravitational Waves from Quantum Hadrodynamics

    Ling-Jun Guo🇨🇳 · Yao Ma🇨🇳 · Yong-Liang Ma🇨🇳 · Ruo-Xi Wu🇨🇳 · Yue-Liang Wu🇨🇳

    White dwarfs, one of the compact objects in the universe, play a crucial role in astrophysical research and provide a platform for exploring nuclear physics. In this work, we extend the relativistic mean field approach by using a Walecka-type quantum hadrodynamics model to capture the intricate structure of white dwarfs. We calculate nuclear properties, Coulomb energy, and photon energy within white dwarfs in a unified framework. By carefully calibrating the model parameters to align with nuclear matter properties, we successfully reproduce the structures of several elements in white dwarfs, such as the isotopes of and , except for the unnaturally deeply bound state He. Furthermore, we predict the characteristics of white dwarfs composed of atom-like units and the gravitational waves stemming from binary white dwarf inspirals incorporating tidal deformability contributions up to the 2.5 post-Newtonian order. These results shed light on the structure of white dwarfs and provide valuable information for future gravitational wave detection. This methodological advancement allows for a cohesive analysis of white dwarfs, neutron stars, and the nuclear pasta within a unified theoretical framework.

    nucl-thastro-ph.HECommun.Theor.Phys.(2025)·3 citations
  4. 04

    Motivations for Early High-Profile FRIB Experiments

    B. Alex Brown🇮🇳 · Alexandra Gade🇮🇳 · S. Ragnar Stroberg🇺🇸 · Jutta Escher🇺🇸 · Kevin Fossez🇺🇸 · Pablo Giuliani🇺🇸 · Calem R. Hoffman🇺🇸 · Witold Nazarewicz🇮🇳 · Chien-Yeah Seng🇺🇸 · Agnieszka Sorensen🇺🇸 · Nicole Vassh🇨🇦 · Daniel Bazin🇮🇳 and 30 other authors

    This white paper is the result of a collaboration by those that attended a workshop at the Facility for Rare Isotope Beams (FRIB), organized by the FRIB Theory Alliance (FRIB-TA), on Theoretical Justifications and Motivations for Early High-Profile FRIB Experiments. It covers a wide range of topics related to the science that will be explored at FRIB. After a brief introduction, the sections address: (II) Overview of theoretical methods, (III) Experimental capabilities, (IV) Structure, (V) Near-threshold Physics, (VI) Reaction mechanisms, (VII) Nuclear equations of state, (VIII) Nuclear astrophysics, (IX) Fundamental symmetries, and (X) Experimental design and uncertainty quantification.

    nucl-thJ.Phys.G(2025)·29 citations
  5. 05

    Investigation of 90,92Zr(n,{\gamma}) 91,93Zr in the s process nucleosynthesis

    Abdul Kabi · Zain Ul Abideen · Jameel-Un Nabi · Dawar Khan

    The neutron capture rates and Maxwellian averaged cross sections (MACS) for 90Zr(n,{\gamma}) 91Zr and 92Zr(n,{\gamma}) 93Zr processes have been computed within the framework of Talys v1.96. The effects of phenomenological nuclear level density (NLD) parameters and the gamma strength functions (GSFs) on Maxwellian averaged cross sections and neutron capture rates are examined both quantitatively and qualitatively. The present model based computed data for MACS and reaction rates gives a good comparison with the existing literature. The fine-tuning of the statistical models nuclear properties (level density and gamma-ray strength) to reproduce experimental data will allow the detailed investigation of the s process network.

    nucl-thastro-ph.SRZ.Naturforsch.A(2024)·1 citation
  6. 06

    Re-analysis of the Gamow-Teller distributions for N=Z nuclei, 24Mg, 28Si, and 32S

    Jameel-Un Nabi · Abdul Kabir · Tuncay Bayram

    The Gamow-Teller (GT) strength distributions of sd shell N=Z nuclei (Mg, Si, and S) are investigated within the framework of proton-neutron quasi particle random phase approximation (pn QRPA) using a deformed basis. The nuclear properties of these special nuclei were investigated by the Relativistic Mean Field (RMF) model. The RMF framework with density-dependent interactions (DD-PC1 and DD-ME2) was employed to compute ground-state deformation parameters (beta 2) using potential energy curves. The values computed from the RMF and the finite range droplet model (FRDM) were employed as a free parameter in the pn QRPA calculation to investigate the resulting GT strength distributions.The present model-based analyses compare well with the observed data.

    nucl-thastro-ph.SRChin.J.Phys.(2024)·3 citations
  7. 07

    Subtleties in the calculation of correlation functions for hot and dense systems

    Sebastian Töpfel🇩🇪 · Andreas Geißel🇩🇪 · Jens Braun🇩🇪

    We discuss subtleties in the calculation of loop integrals in studies of hot and dense systems as they appear in both perturbative and non-perturbative approaches. To be specific, we address subtleties which appear in situations where the order of integration, differentiation, and limit processes plays a crucial role. For example, this applies to computations of the effective action and the computation of momentum-dependent correlation functions. In particular, the zero-temperature limit is delicate in systems with fermions because of the presence of discontinuities at the Fermi surface. We provide a general discussion of scenarios where the computation and evaluation of loop integrals in the context of relativistic theories requires particular attention as a change of the order of the involved mathematical operations may lead to a different result. Our general considerations are then illustrated with the aid of concrete examples, namely by the computation of masses from fully momentum-dependent correlation functions in the context of the Gross-Neveu-Yukawa model and quantum electrodynamics.

    nucl-thhep-thPRD(2025)·4 citations
  8. 08

    Study of /EC-decay properties of shell nuclei using nuclear shell model

    Surender · Vikas Kumar · Praveen C. Srivastava

    Our study employs the nuclear shell model to systematically compute the half-lives of -decay for nuclei in the mass range of , encompassing the majority of shell nuclei. This analysis utilizes the USDB and SDNN Hamiltonians. The theoretical outcomes contain calculations of various parameters such as -values, half-lives, excitation energy, log values, and branching ratios. We explore these results with axial-vector coupling constant for weak interactions, denoted as , and value . We perform calculations of Gamow Teller matrix elements for 116 decay processes to calculate the quenching factor; we found a quenching factor of for the USDB interaction and for the SDNN interaction. We have also calculated superallowed transitions for seven nuclei. Further, we have also included the electron capture phase space factor for the required nuclei to calculate the half-lives. This inclusion leads to small contribution in results, particularly for nuclei where electron capture (EC) plays a significant role. The overall results are in agreement with the experimental data.

    nucl-thAnnals Phys.(2024)·4 citations
  9. 09

    Tunnelling amplitudes through localised external potentials from Feynman diagram summation

    Rosemary Zielinski🇦🇺 · Cedric Simenel🇦🇺 · Patrick McGlynn🇦🇺

    Currently there is no general theory of quantum tunnelling of a particle through a potential barrier which is compatible with QFT. We present a complete calculation of tunnelling amplitudes for a scalar field for some simple potentials using quantum field-theoretic methods. Using the perturbative S-matrix formalism, starting with the Klein-Gordon Lagrangian, we show that an infinite summation of Feynman diagrams can recover tunnelling amplitudes consistent with relativistic quantum mechanics. While this work does not include many-particle effects arising from a fully quantised QFT, it is necessary to investigate QFT corrections to tunnelling amplitudes.

    hep-thnucl-thEPJC(2024)·5 citations
  10. 10

    Quantum corrections to tunnelling amplitudes of neutral scalar fields

    Rosemary Zielinski🇦🇺 · Patrick McGlynn🇦🇺 · Cedric Simenel🇦🇺

    Though theoretical treatments of quantum tunnelling within single-particle quantum mechanics are well-established, at present, there is no quantum field-theoretic description (QFT) of tunnelling. Due to the single-particle nature of quantum mechanics, many-particle effects arising from quantum field theory are not accounted for. Such many-particle effects, including pair-production, have proved to be essential in resolving the Klein-paradox. This work seeks to determine how quantum corrections affect the tunnelling probability through an external field. We investigate a massive neutral scalar field, which interacts with an external field in accordance with relativistic quantum mechanics. To consider QFT corrections, we include another massive quantised neutral scalar field coupling to the original via a cubic interaction. This study formulates an all-order recursive expression for the loop-corrected scalar propagator, which contains only the class of vertex-corrected Feynman diagrams. This equation applies for general external potentials. Though there is no closed-form analytic solution, we also demonstrate how to approximate the QFT corrections if a perturbative coupling to the quantised field is assumed.

    hep-thnucl-thEPJC(2024)·3 citations
  11. 11

    QCD deconfinement transition line up to MeV from finite volume lattice simulations

    Szabolcs Borsanyi🇩🇪 · Zoltan Fodor🇩🇪 · Jana N. Guenther🇩🇪 · Paolo Parotto🇮🇹 · Attila Pasztor🇭🇺 · Ludovica Pirelli🇩🇪 · Kalman K. Szabo🇩🇪 · Chik Him Wong🇩🇪

    The QCD cross-over line in the temperature () -- baryo-chemical potential () plane has been computed by several lattice groups by calculating the chiral order parameter and its susceptibility at finite values of . In this work we focus on the deconfinement aspect of the transition between hadronic and Quark Gluon Plasma (QGP) phases. We define the deconfinement temperature as the peak position of the static quark entropy () in , which is based on the renormalized Polyakov loop. We extrapolate based on high statistics finite temperature ensembles on a lattice to finite density by means of a Taylor expansion to eighth order in (NNNLO) along the strangeness neutral line. For the simulations the 4HEX staggered action was used with 2+1 flavors at physical quark masses. In this setup the phase diagram can be drawn up to unprecedentedly high chemical potentials. Our results for the deconfinement temperature are in rough agreement with phenomenological estimates of the freeze-out curve in relativistic heavy ion collisions. In addition, we study the width of the deconfinement crossover. We show that up to MeV, the deconfinement transition gets broader at higher densities, disfavoring the existence of a deconfinement critical endpoint in this range. Finally, we examine the transition line without the strangeness neutrality condition and observe a hint for the narrowing of the crossover towards large .

    hep-lathep-phnucl-thPRD(2024)·28 citations
  12. 12

    Relations Between Anomalous Dimensions in the Regge Limit

    Ira Z. Rothstein🇺🇸 · Michael Saavedra🇺🇸

    We extend the recent formalism developed for computing rapidity anomalous dimension of form factors using unitarity to the problem of high-energy near forward scattering. By combining the factorization of scattering in the effective field theory (EFT) for Glauber operators with definite signature amplitudes, we derive an expression that relates anomalous dimensions (including Regge trajectories) to cut amplitudes, leading to significant computational simplifications. We demonstrate this explicitly by computing the one and two-loop Regge trajectories. Our formalism can also be used to bootstrap anomalous dimensions of operators not related by symmetries. As an example, we show that the full anomalous dimensions (including both the Regge pole and cut pieces) of the two Glauber operator anti-symmetric octet operator, can be determined from the anomalous dimension of the single Glauber exchange operator. Many other such relations exist between other color channels at each order in .

    hep-phhep-thnucl-thJHEP(2025)·8 citations
  13. 13

    Magnetic coupling through flux branching of adjacent type-I and -II superconductors in a neutron star

    K. H. Thong · A. Melatos

    The inner and outer cores of neutron stars are believed to contain type-I and -II proton superconductors, respectively. The type-I superconductor exists in an intermediate state, comprising macroscopic flux-free and flux-containing regions, while the type-II superconductor is flux-free, except for microscopic, quantized flux tubes. Here, we show that the inner and outer cores are coupled magnetically, when the macroscopic flux tubes subdivide dendritically into quantized flux tubes, a phenomenon called flux branching. An important implication is that up to of energy are required to separate a quantized flux tube from its progenitor macroscopic flux tube, where is the length of the macroscopic flux tube. Approximating the normal-superconducting boundary as sharp, we calculate the magnetic coupling energy between a quantized and macroscopic flux tube due to flux branching as a function of, , the radius of the type-I inner core divided by the radius of the type-II outer core. Strong coupling delays magnetic field decay in the type-II superconductor. For an idealised inner core containing only a type-I proton superconductor and poloidal flux, and in the absence of ambipolar diffusion and diamagnetic screening, the low magnetic moments () of recycled pulsars imply .

    astro-ph.HEcond-mat.quant-gascond-mat.supr-congr-qc+1MNRAS(2024)·2 citations
  14. 14

    A New-Old Approach to Composite Scalars with Chiral Fermion Constituents

    Christopher T. Hill🇺🇸

    We develop a dynamical, Lorentz invariant theory of composite scalars in configuration space consisting of chiral fermions, interacting by the perturbative exchange of a massive "gluon" of coupling and mass (the coloron model). The formalism is inspired by, but goes beyond, old ideas of Yukawa and the Nambu-Jona-Lasinio (NJL) model. It yields a non-pointlike internal wave-function of the bound state, , which satisfies a Schrödinger-Klein-Gordon (SKG) equation with eigenvalue . For super-critical coupling, , we have leading to spontaneous symmetry breaking. The binding of chiral fermions is semiclassical, and not loop-level as in NJL. The mass scale is determined by the interaction as in NJL. We mainly focus on the short-distance, large limit, yielding an NJL pointlike interaction, but the bound state internal wave-function, , remains spatially extended and dilutes . This leads to power-law suppression of the induced Yukawa and quartic couplings and requires radically less fine-tuning of a hierarchy than does the NJL model. We include a discussion of loop corrections of the theory. A realistic top--condensation model appears possible.

    hep-phhep-exhep-thnucl-thNPB(2025)·3 citations
  15. 15

    Exclusive rare semileptonic decays of and mesons in the relativistic independent quark model

    Kalpalata Dash🇮🇳 · P. C. Dash🇮🇳 · R. N. Panda🇮🇳 · Susmita Kar🇮🇳 · N. Barik🇮🇳

    We investigate the exclusive rare semileptonic decays: () in the framework of relativistic independent quark (RIQ) model based on an average flavor independent confining potential in equally mixed scalar-vector harmonic form. The invariant weak form factors, parametrising the matrix elements between participating meson states are calculated in the parent meson rest frame. The momentum transfer dependence of the form factors is reliably determined in the whole accessible kinematical range: . Our predicted branching fractions for , , and , obtained in order of , , and , respectively are in reasonable agreement with other Standard Model predictions and Lattice QCD results. The averaged values of the lepton polarization asymmetries for decay modes are obtained as =-0.97, =-0.972, =-0.224, =-0.275 and =-0.194.

    hep-phnucl-thPRD(2024)·1 citation

Affiliations

first authorsco-authorsvia INSPIRE