Nuclear transition matrix elements for neutrinoless double-β decay of 76Ge isotope within PHFB approach

被引:3
|
作者
Rath, P. K. [1 ]
Kumar, A. [1 ]
Chandra, R. [2 ]
Gautam, R. [2 ]
Raina, P. K. [3 ]
Dixit, B. M. [4 ]
机构
[1] Univ Lucknow, Dept Phys, Lucknow 226007, Uttar Pradesh, India
[2] Babasaheb Bhimrao Ambedkar Univ, Dept Phys, Lucknow 226025, Uttar Pradesh, India
[3] Indian Inst Technol Roper, Dept Phys, Rupnagar 140001, Punjab, India
[4] SRM Univ, Fac Phys Sci, Barabanki 225013, India
来源
INTERNATIONAL JOURNAL OF MODERN PHYSICS E | 2019年 / 28卷 / 11期
关键词
PHFB model; neutrinoless double beta decay; nuclear transition matrix elements; SUPPRESSION;
D O I
10.1142/S0218301319500964
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
Employing projected-Hartree-Fock-Bogoliubov (PHFB) model, nuclear transition matrix elements (NTMEs) M-(K) for the neutrinoless double-beta(-) decay of Ge-76 isotope are calculated within mechanisms involving light as well as heavy Majorana neutrinos, and classical Majorons. By considering the spin-tensor decomposition of realistic KUO and empirical JUN45 effective two-body interactions, it is noticed that the effect due to SRC on NTMEs M-(0 nu) and M-(0N) involving the exchange of light and heavy Majorana neutrinos, respectively, is maximally incorporated by the central part of the effective two-body interaction, which varies by a small amount with the inclusion of spin-orbit and tensor components. Presently, the model-dependent uncertainties in the average NTMEs (M) over bar ((0 nu)) and (M) over bar ((0N)) turn out to be about 10% and 37%, respectively.
引用
收藏
页数:12
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