Radiative pion capture by a nucleon

被引:24
作者
Fearing, HW
Hemmert, TR
Lewis, R
Unkmeir, C
机构
[1] TRIUMF, Vancouver, BC V6T 2A3, Canada
[2] Forschungszentrum Julich, Inst Kernphys, D-52425 Julich, Germany
[3] Univ Regina, Dept Phys, Regina, SK S4S 0A2, Canada
[4] Johannes Gutenberg Univ Mainz, Inst Kernphys, D-55099 Mainz, Germany
来源
PHYSICAL REVIEW C | 2000年 / 62卷 / 05期
关键词
D O I
10.1103/PhysRevC.62.054006
中图分类号
O57 [原子核物理学、高能物理学];
学科分类号
070202 ;
摘要
The differential cross sections for pi (-)p-->gamman and pi (+)n-->gammap are computed up to O(p(3)) in heavy baryon chiral perturbation theory (HBChPT). The expressions at O(p) and O(p(2)) have no free parameters. There are three unknown parameters at O(p(3)), low energy constants of the HBChPT Lagrangian, which are determined by fitting to experimental data. Two acceptable fits are obtained, which can be separated by comparing with earlier dispersion relation calculations of the inverse process. Expressions for the multipoles, with emphasis on the p-wave multipoles, are obtained and evaluated at threshold. Generally the results obtained from the best of the two fits are in good agreement with the dispersion relation predictions.
引用
收藏
页码:540061 / 5400610
页数:10
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