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Neutrinolessββdecay transition matrix elements within mechanisms involving light Majorana neutrinos, classical Majorons, and sterile neutrinos

2013/08/31 by P. K. Rath, R. Chandra, K. Chaturvedi +4 · 1 citation
Chemistry · Physics and Astronomy · #Biology #Chemistry #MAJORANA #Matrix (chemical analysis) #Neutrino #Neutrino Physics Research #Nuclear physics #Nuclear physics research studies #Pairing #Parametrization (atmospheric modeling) #Particle physics #Particle physics theoretical and experimental studies #Physics #Quantum mechanics #Type (biology) #nucl-th

paper · pdf · doi:10.1103/physrevc.88.064322

published as Phys. Rev. C 88, 064322 (2013)

openalex publication_date 2013/12/20 · arxiv created 2013/12/23 · arxiv updated 2015/06/16 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05

Abstract

In the projected-Hartree-Fock-Bogoliubov (PHFB) model, uncertainties in the nuclear transition matrix elements for the neutrinoless double-\ensuremathβ decay of \phantom\rule4pt0ex94,96Zr, 98,100Mo, 104Ru, 110Pd, 128,130Te, and 150Nd isotopes within mechanisms involving light Majorana neutrinos, classical Majorons, and sterile neutrinos are statistically estimated by considering sets of 16 (24) matrix elements calculated with four different parametrizations of the pairing plus multipolar type of effective two-body interaction, two sets of form factors, and two (three) different parametrizations of Jastrow type of short-range correlations. In the mechanisms involving the light Majorana neutrinos and classical Majorons, the maximum uncertainty is about 15% and in the scenario of sterile neutrinos, it varies in between approximately 4 (9)%--20 (36)% without(with) Jastrow short range correlations with the Miller-Spencer parametrization, depending on the considered mass of the sterile neutrinos.

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