MAGNETIC INTERACTION BETWEEN RELATIVISTIC ATOMIC ELECTRONS AND PARITY NONCONSERVING NUCLEAR MOMENTS

被引：5
|
作者：
FLAMBAUM, VV
HANHART, C
机构：
[1] School of Physics, University of New South Wales, Kensington, NSW 2033
来源：
PHYSICAL REVIEW C | 1993年 / 48卷 / 03期
关键词：
D O I：
10.1103/PhysRevC.48.1329
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：
Parity nonconserving nuclear forces induce electromagnetic currents and nuclear moments of the wrong parity (e.g., anapole moment). The interaction between atomic electrons and these currents is considered taking into account finite nuclear size and relativistic effects. The formula has been derived which allows one to separate the atomic and nuclear problems. The result can be approximately expressed as the interaction of an electron with a pointlike nuclear anapole moment times a correction factor [1 - 0.3(Zalpha)2]. As an illustration we use a simple model to calculate the distribution of the parity-violating electromagnetic current, magnetic field, and vector potential.
引用
收藏
页码：1329 / 1334
页数：6
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