Uncertainties in nuclear transition matrix elements for neutrinoless ββ decay: The heavy Majorana neutrino mass mechanism

被引:23
|
作者
Rath, P. K. [1 ]
Chandra, R. [2 ,3 ]
Raina, P. K. [3 ,4 ]
Chaturvedi, K. [5 ]
Hirsch, J. G. [6 ]
机构
[1] Univ Lucknow, Dept Phys, Lucknow 226007, Uttar Pradesh, India
[2] Babasaheb Bhimrao Ambedkar Univ, Dept Appl Phys, Lucknow 226025, Uttar Pradesh, India
[3] Indian Inst Technol, Dept Phys & Meteorol, Kharagpur 721302, W Bengal, India
[4] Indian Inst Technol, Dept Phys, Rupnagar 140001, Punjab, India
[5] Bundelkhand Univ, Dept Phys, Jhansi 284128, Uttar Pradesh, India
[6] Univ Nacl Autonoma Mexico, Inst Ciencias Nucl, Mexico City 04510, DF, Mexico
来源
PHYSICAL REVIEW C | 2012年 / 85卷 / 01期
关键词
SHELL-MODEL; DEFORMATION; PARTICLE; SUPPRESSION; SEARCH; LEPTON;
D O I
10.1103/PhysRevC.85.014308
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 four different parametrizations of the pairing plus the multipolar type of effective two-body interaction and three different parametrizations of the Jastrow type of short-range correlations, the uncertainties in the nuclear transition matrix elements M-N((0 nu)) due to the exchange of heavy Majorana neutrino for the 0(+) -> 0(+) transition of neutrinoless double beta decay of Zr-94, Zr-96, Mo-98, Mo-100, Ru-104, Pd-110, Te-128,Te-130, and Nd-150 isotopes in the PHFB model are estimated to be around 35%. Excluding the nuclear transition matrix elements calculated with the Miller-Spencer parametrization of Jastrow short-range correlations, the uncertainties are found to be smaller than 20%.
引用
收藏
页数:9
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