PaperPanorama

Nuclear Theory·nucl-th

Friday·February 16, 2018

9 papers5 primary·4 cross-listed

  1. 06

    New high-spin structure and possible chirality in In

    M. Wang · Y. Y. Wang · L. H. Zhu · B. H. Sun · G. L. Zhang · L. C. He · W. W. Qu · F. Wang · T. F. Wang · Y. Y. Chen · C. Xiong · J. Zhang and 11 other authors

    High-spin structure of In has been investigated with the Mo(N, 5)In reaction at a beam energy of 78 MeV using the in-beam spectroscopic method. The level scheme of In has been modified considerably and extended by 46 new -rays to the highest excited state at 8.979 MeV and =(45/2). The new level scheme consists of eight bands, six of which are identified as dipole bands. The configurations have been tentatively assigned with the help of the systematics of neighboring odd- indium isotopes and the experimental aligned angular momenta. The dipole bands are then compared with the titled axis cranking calculation in the framework of covariant density function theory (TAC-CDFT). The results of theoretical calculation based on the configurations, which involve one proton hole at the orbital and two or four unpaired neutrons at , and orbitals, show that the shape of In undergoes an evolution on both and deformations and possible chirality is suggested in In.

    nucl-exnucl-thPRC(2018)·10 citations
  2. 07

    Magnetic moments of the lowest-lying singly heavy baryons

    Ghil-Seok Yang🇰🇷 · Hyun-Chul Kim🇰🇷

    A light baryon is viewed as valence quarks bound by meson mean fields in the large limit. In much the same way a singly heavy baryon is regarded as valence quarks bound by the same mean fields, which makes it possible to use the properties of light baryons to investigate those of the heavy baryons. A heavy quark being regarded as a static color source in the limit of the infinitely heavy quark mass, the magnetic moments of the heavy baryon are determined entirely by the chiral soliton consisting of a light-quark pair. The magnetic moments of the baryon sextet are obtained by using the parameters fixed in the light-baryon sector. In this mean-field approach, the numerical results of the magnetic moments of the baryon sextet with spin are just 3/2 larger than those with spin . The magnetic moments of the bottom baryons are the same as those of the corresponding charmed baryons.

    hep-phhep-exnucl-thPLB(2018)·39 citations
  3. 08

    Shannon entropy and particle decays

    Pedro Carrasco Millan🇪🇸 · M. Angeles Garcia-Ferrero🇪🇸 · Felipe J. Llanes-Estrada🇪🇸 · Ana Porras Riojano🇪🇸 · Esteban M. Sanchez Garcia🇪🇸

    We deploy Shannon's information entropy to the distribution of branching fractions in a particle decay. This serves to quantify how important a given new reported decay channel is, from the point of view of the information that it adds to the already known ones. Because the entropy is additive, one can subdivide the set of channels and discuss, for example, how much information the discovery of a new decay branching would add; or subdivide the decay distribution down to the level of individual quantum states (which can be quickly counted by the phase space). We illustrate the concept with some examples of experimentally known particle decay distributions.

    hep-phhep-exnucl-thNPB(2018)·11 citations
  4. 09

    Equation for the Nakanishi weight function using the inverse Stieltjes transform

    V.A. Karmanov🇷🇺 · J. Carbonell🇫🇷 · T. Frederico🇧🇷

    The bound state Bethe-Salpeter amplitude was expressed by Nakanishi in terms of a smooth weight function g. By using the generalized Stieltjes transform, we derive an integral equation for the Nakanishi function g for a bound state case. It has the standard form g= Vg, where V is a two-dimensional integral operator. The prescription for obtaining the kernel V starting with the kernel K of the Bethe-Salpeter equation is given.

    hep-phnucl-thFew Body Syst.(2018)·1 citation

Affiliations

first authorsco-authorsvia INSPIRE