PaperPanorama

Nuclear Theory·nucl-th

Friday·September 2, 2022

7 papers3 primary·4 cross-listed

  1. 01

    Variational Monte Carlo Calculations of n+3H Scattering

    Abraham R. Flores · Kenneth M. Nollett

    A paramount goal in the field of nuclear physics is to unify ab-initio treatments of bound and unbound states. The position-space quantum Monte Carlo (QMC) methods have a long history of successful bound state calculations in light systems but so far have seen very little application to unbound systems. Here we introduce a numerical method to improve the efficiency and accuracy of unbound-state calculations in QMC, and as an initial application we compute scattering observables for the neutron-triton system using variational Monte Carlo (VMC) wave functions. The method consists of inferring long-range amplitudes in the wave function from integrals over the short-ranged region where all the particles interact. This approach using integral relations is well established in the literature; here we develop it for the QMC framework. We validate our code with a consistency check between short-range spectroscopic overlap functions computed from direct evaluation and from the integral relations; scattering amplitudes are long-range asymptotics of those overlaps. Comparison against published benchmark calculations using the same potential demonstrates that the integral method, when applied to the current VMC wave functions, produces more accurate scattering observables than direct evaluation from the same variational wave function. However, it still differs noticeably from exact results. We then present phase shifts and mixing parameters for the neutron-triton system using various interactions. Application of the integral method here paves the way for its use in Green's function Monte Carlo (GFMC) calculations. In GFMC the wave functions are more precise, but high-precision convergence of their tails is slow, and there are additional difficulties in reading out amplitudes. The integral methods will address both of those remaining problems.

    nucl-thPRC(2023)·15 citations
  2. 02

    Imprints of clustering in multiplicity fluctuations

    A. Bazgir🇵🇱 · V.Z. Reyna Ortiz🇵🇱 · M. Rybczynski🇵🇱 · U. Shah🇵🇱 · Z. Wlodarczyk🇵🇱

    In this paper, we investigate the multiplicity fluctuations of charged particles observed in high-energy nuclear collisions and relate them to the size of hadronizing systems which happen during such processes. We use the average multiplicities and variances of multiplicity distributions of charged particles produced in centrality selected collisions of relativistic heavy-ion nuclei to evaluate the dynamic variable and study its dependence on the size of colliding nuclei. We connect the observed system-size dependence of multiplicity fluctuations with the clustering phenomena and the finiteness of the hadronizing sources and the thermal bath.

    nucl-thhep-phEPJA(2023)·0 citations
  3. 03

    Directed flow in relativistic resistive magneto-hydrodynamic expansion for symmetric and asymmetric collision systems

    Kouki Nakamura🇯🇵 · Takahiro Miyoshi🇯🇵 · Chiho Nonaka🇯🇵 · Hiroyuki R. Takahashi🇯🇵

    We construct a dynamical model for high-energy heavy-ion collision based on the relativistic resistive magneto-hydrodynamic framework. Using our newly developed (3+1)-dimensional relativistic resistive magneto-hydrodynamics code, we investigate magneto-hydrodynamic expansion in symmetric and asymmetric collision systems as a first application to high-energy heavy-ion collisions. As a realistic initial condition for electromagnetic fields, we consider the solutions of the Maxwell equations with the source term of point charged particles moving in the direction of the beam axis, including finite constant electrical conductivity of the medium. We evaluate the directed flow in the symmetric and asymmetric collisions at RHIC energy. We find a significant effect of finite electrical conductivity on the directed flow in the asymmetric collision system. We confirm that a certain amount of energy transfer by dissipation associated with Ohmic conduction occurs in the asymmetric collision system because of asymmetry of the electric field produced by two different colliding nuclei. Because this energy transfer makes the pressure gradient of the medium flatter, the growth of directed flow decreases.

    nucl-thhep-phnucl-exPRC(2023)·18 citations

Affiliations

first authorsco-authorsvia INSPIRE