PaperPanorama

Nuclear Theory·nucl-th

Thursday·October 23, 2025

11 papers4 primary·7 cross-listed

  1. 01

    Connecting ground-state properties of Li to each other and to scattering data

    Chloë Hebborn🇫🇷 · Carl R. Brune🇺🇸 · Daniel R. Phillips🇺🇸

    We examine the relationship between the Asymptotic Normalization Coefficient (ANC) of Li and other low-energy observables in the -deuteron system. Our analysis uses a set of calculations carried out within the {\it ab initio} No Core Shell Model with Continuum (NCSMC) using a variety of inter-nucleon interactions and basis sizes, and yielding Li deuteron separation energies between 1.3 and 1.8 MeV [Phys. Rev. Lett. 129, 042503 (2022)]. These NCSMC calculations show that the square of the ANC is strongly correlated with the separation energy over this range. In this work, we investigate the origin of this correlation using the phenomenological -matrix, a single-channel potential and a perturbative approach. We show that this correlation occurs because the depth of the -deuteron central potential changes by only a small relative amount as the separation energy varies. We then investigate if the ANC can be accurately extracted from -deuteron phase shifts in an ideal case in which low-energy data are available and there are no experimental errors. We find that both -matrix and Coulomb-modified effective-range theory (CM-ERE) yield extracted ANCs close to, although not exactly equal to, the true value, provided the extrapolation is constrained by the known position of the bound-state pole and at least three terms are included in the fit function. The -matrix approach converges faster than the CM-ERE as the number of parameters increases and is also more robust against the inclusion of low-energy and high-energy phase shift data. Finally, our study also shows that a naive quantification of uncertainties by comparing different truncations used in both theories is not accurate, and suggests the accuracy of ANCs extracted from phase shift data needs further investigation.

    nucl-thJ.Phys.G(2026)·0 citations
  2. 02

    Resolving the spurious-state problem in Dirac equation by using the staggered-grid method

    Lingfeng Li🇨🇳 · Hong Shen🇨🇳 · Jinniu Hu🇨🇳 · Ying Zhang🇨🇳

    Discretizing the Dirac equation on a uniform grid with the central difference formula often generates spurious states. We propose a staggered-grid scheme in the framework of the finite-difference method that suppresses these spurious states without introducing Wilson terms or ad-hoc filtering. In this approach, the large and small components of the Dirac equation are placed on interlaced nodes, and the first-order derivatives are evaluated between staggered points, yielding a Hamiltonian that breaks the unitary transformation between and . Benchmarks with the nuclear Woods-Saxon potentials demonstrate one-to-one agreement with the eigenvalues obtained from shooting method and asymmetric finite-difference method, rapid convergence for weakly bound states, and reduced box-size sensitivity. The method retains the simplicity of central differences and standard matrix diagonalization, while naturally extending to higher-order and multi-dimension systems. It provides a compact and efficient tool for relativistic bound-state and scattering calculations.

    nucl-thPRC(2026)·0 citations
  3. 03

    The universal size compression effect of nucleon pair in finite nuclei

    Qing Zhao🇨🇳 · Masaaki Kimura🇯🇵 · Bo Zhou🇨🇳 · Seung-heon Shin🇯🇵

    We systematically investigate the size evolution of the di-neutron (2n), di-proton (2p), and deuteron (d) in 6He, 14Be, 17B, 6Be, 17Ne, and 6Li using microscopic calculations. Remarkably, all nucleon pairs exhibit a universal size compression at the nuclear surface, regardless of their species and binding energies. These features correspond to the BCS- and BEC-like nucleon pairs, which recent experimental techniques can further investigate.

    nucl-th0 citations
  4. 04

    Kinetic energy of fission fragments within a dynamical model

    S. Takagi🇯🇵 · Y. Aritomo🇯🇵 · K. Nakajima🇯🇵 · K. Okada🇯🇵 · K. Hirose🇯🇵 · K. Nishio🇯🇵

    Kinetic energy of individual fission fragment for actinide nuclei is, for example, important for evaluating the prompt-neutron spectrum in the laboratory system. It is experimentally known that kinetic energy for each fragment is constant at about 100 MeV for light fragments and that for heavy fragments decreases linearly with mass number. Most of the theoretical studies carried out so far attempted to calculate the total kinetic energy of both fragments, i.e. sum of the energies of two fragments, but the kinetic energy of each fragment was not analyzed in detail as far as we recognize. We have calculated them in thermal-neutron induced fission of with a dynamical model using Langevin equations within a three-dimensional two-center parametrization. Also fission of was investigated. It is calculated from the Coulomb energy at the scission point and the pre-scission kinetic energy. It is found that the pre-scission kinetic energy has about 2-4% contribution in the kinetic energy. The calculated results reproduce the trend of the experimental data.

    nucl-thPRC(2025)·0 citations

Affiliations

first authorsco-authorsvia INSPIRE