中文

$^{22}$Na中$2_1^+ \to 3_1^+$的γ宽度与二类流

核实验 2018-10-09 v1

摘要

先前对22^{22}Na β\beta衰变中βγ\beta-\gamma方向系数的测量被用于提取反冲阶形状因子。数据表明该衰变需要一个显著的诱导张量矩阵元。这一结论很大程度上依赖于一个标准模型允许的弱磁形状因子,该因子是利用22^{22}Na中类似的21+31+2_1^+\to3_1^+ γ\gamma分支的比未发表值确定的,并进一步假设该跃迁由其同位旋矢量M1M1分量主导。我们首次明确确定22^{22}Na中21+31+2_1^+ \to 3_1^+分支比为0.45(8)%0.45(8)\%。利用守恒矢量流(CVC)假说,我们的分支比确定22^{22}Na β\beta衰变的弱磁形状因子为b/Ac1=8.7(1.1)|b/Ac_1| = 8.7(1.1)。结合βγ\beta-\gamma角关联系数,我们得到该衰变的一个大诱导张量形状因子,其仍与理论预测不符。给出了两种合理的解释。

关键词

引用

@article{arxiv.1701.05545,
  title  = {The $2_1^+ \to 3_1^+$ gamma width in $^{22}$Na and second class currents},
  author = {S. Triambak and L. Phuthu and A. García and G. C. Harper and J. N. Orce and D. A. Short and S. P. R. Steininger and A. Diaz Varela and R. Dunlop and D. S. Jamieson and W. A. Richter and G. C. Ball and P. E. Garrett and C. E. Svensson and C. Wrede},
  journal= {arXiv preprint arXiv:1701.05545},
  year   = {2018}
}

备注

Submitted to Phys. Rev. C