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RELATIVISTIC MEAN-FIELD APPROACH TO ANAPOLE MOMENT - ATOMIC PARITY-VIOLATING HYPERFINE TRANSITIONS

机译:相对惯性矩的平均位移法-违反原子奇偶校验的超精细转变

摘要

A generalized formula of nuclear anapole moment-is derived using the current relativistic nuclear approach. The Dirac spin magnetization and the anomalous spin magnetization contributions to anapole moment are shown to be proportional to the second moment of respective magnetizations. The valence nucleon effective g(l)(g(a)) factors in a nucleus are obtained from the different phenomenological generalizations of relativistic nuclear magnetic moment. The unitary transformation approach is used to derive the parity nonconserving (PNC) perturbed wave functions. In the case of gl parametrization, the anomalous spin magnetization and pion contributions to anapole moment are nearly two and three times the Dirac magnetization contribution respectively; while for g(a) parametrization, all the three contributions are of the same order of magnitude. Using these calculated values of anapole moment and available atomic structure data from published literature, the Cs-133 pNC hyperfine amplitudes are calculated. The results are closer to the experimental data, particularly when the measured value of ImEP1(p.v.)/beta is used. The optical rotation angles induced by nuclear spin dependent PNC interaction are also calculated.
机译:使用当前的相对论核方法,可以得出核回极矩的广义公式。 Dirac自旋磁化强度和反自旋磁化强度对偶极矩的贡献显示为与各自磁化强度的第二矩成比例。原子核中的价原子核有效g(l)(g(a))因子是从相对论核磁矩的不同现象学概括中获得的。 unit变换方法用于导出奇偶非保守(PNC)扰动波函数。在gl参数化的情况下,异常自旋磁化强度和pion对偶极矩的贡献分别接近Dirac磁化强度的两倍和三倍。而对于g(a)参数化,这三个贡献都处于相同的数量级。使用这些偶极矩的计算值和公开文献中的可用原子结构数据,可以计算出Cs-133 pNC超精细振幅。结果更接近实验数据,尤其是当使用ImEP1(p.v。)/ beta的测量值时。还计算了由核自旋相关的PNC相互作用引起的旋光角。

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