vix.ing · top · new · best · stats · spec

Study of P-wave excitations of observed charmed strange baryons

2017/09/30 by Dan-Dan Ye, Dandan Ye, Ze Zhao +1 · 3 citations
Chemistry · Physics and Astronomy · #Atomic physics #Chemistry #Crystallography #Excited state #High-Energy Particle Collisions Research #Order (exchange) #Particle physics #Particle physics theoretical and experimental studies #Physics #Quantum Chromodynamics and Particle Interactions #hep-ph

paper · pdf · doi:10.1103/physrevd.96.114009

published as Phys. Rev. D 96, 114009 (2017) · 10 pages, 1 figure, 11 tables, RevTex, to appear in Phys.Rev.D

openalex created_date 2017/09/15 · arxiv created 2017/11/16 · openalex publication_date 2017/12/13 · arxiv updated 2017/12/20 · openalex updated_date 2026/08/05

Abstract

Many excited charmed strange baryons such as \mathrm\ensuremathΞc(2790), \mathrm\ensuremathΞc(2815), \mathrm\ensuremathΞc(2930), \mathrm\ensuremathΞc(2980), \mathrm\ensuremathΞc(3055), \mathrm\ensuremathΞc(3080), and \mathrm\ensuremathΞc(3123) have been observed. In order to understand their internal structure and to determine their spin parities, the strong decay properties of these baryons as possible P-wave excited \mathrm\ensuremathΞc candidates have been systematically studied in a 3P0 model. The configurations and JP assignments of \mathrm\ensuremathΞc(2790), \mathrm\ensuremathΞc(2815), \mathrm\ensuremathΞc(2930), \mathrm\ensuremathΞc(2980), \mathrm\ensuremathΞc(3055), \mathrm\ensuremathΞc(3080), and \mathrm\ensuremathΞc(3123) have been explored based on recent experimental data. In our analyses, \mathrm\ensuremathΞc(3055), \mathrm\ensuremathΞc(3080), and \mathrm\ensuremathΞc(3123) seem impossible to be the P-wave excited \mathrm\ensuremathΞc. \mathrm\ensuremathΞc(2790), \mathrm\ensuremathΞc(2815), \mathrm\ensuremathΞc(2930), and \mathrm\ensuremathΞc(2980) may be the P-wave excited \mathrm\ensuremathΞc. In particular, \mathrm\ensuremathΞc(2790) and \mathrm\ensuremathΞc(2815) are very possibly the P-wave excited \mathrm\ensuremathΞc1(1/2^\ensuremath-) and \mathrm\ensuremathΞc1(3/2^\ensuremath-), respectively. \mathrm\ensuremathΞc(2980) may be the P-wave excited \mathrm\ensuremathΞc1^\ensuremath'((1)/(2)^\ensuremath-). \mathrm\ensuremathΞc(2930) may be the P-wave \mathrm\ensuremathΞc0^\ensuremath'((1)/(2)^\ensuremath-), \stackrel\texttildelow\mathrm\ensuremathΞc0((1)/(2)^\ensuremath-), \mathrm\ensuremathΞc2^\ensuremath'((3)/(2)^\ensuremath-), \mathrm\ensuremathΞc2^\ensuremath'((5)/(2)^\ensuremath-), \stackrel\texttildelow\mathrm\ensuremathΞc2((3)/(2)^\ensuremath-), or \stackrel\texttildelow\mathrm\ensuremathΞc2((5)/(2)^\ensuremath-). Furthermore, some branching fraction ratios related to the internal structure and quark configuration of P-wave \mathrm\ensuremathΞc have also been computed. Measurements of these ratios in the future will be helpful to understand these excited \mathrm\ensuremathΞc.

Citations

Cited by