ÚTEFČVUT Ústav technické a experimentální fyziky ČVUT v PrazeInstitute of Experimental and Applied Physics, CTU in Prague

Double Beta Decay of 48Ca within EMPM and STDA methods

NázevTitle
Double Beta Decay of 48Ca within EMPM and STDA methodsDouble Beta Decay of 48Ca within EMPM and STDA methods
Druh výsledkuResult type
Příspěvek ve sborníkuProceedings paper
AutořiAuthors
P. Veselý, G. De Gregorio, D. Denisova, F. Knapp, F. Šimkovic
Klíčová slovaKeywords
double beta decay, 48Ca, nuclear matrix element, neutrinoless double beta decay, Second Tamm-Dancoff Approximation, Equation of Motion Phonon Method (EMPM)
KonferenceConference
14th International Spring Seminar on Nuclear Physics: "Cutting-edge developments in nuclear structure physics" (Ischia, Italy, 2025-05-19)
DOIDOI
10.1051/epjconf/202534201030
Časopis / citaceJournal / citation
EPJ Web of Conferences 342, 01030 (2025) · ISSN 2100-014X
RokYear
2025
JazykLanguage
eng
ZáznamyRecords
ProjektProject
Zkoumaní vlastností neutrin prostřednictvím dvojitého beta rozpadu: Souhra teorie a experimentuExploring the Properties of Neutrinos through Double Beta Decay: An Interplay between Theory and Experiment
Plný text (open access)Full text (open access)
https://www.epj-conferences.org/articles/epjconf/pdf/2025/27/epjconf_NuclearPhy…
Citace ke staženíDownload citation
TXT · BibTeX

AbstraktAbstract

The calculation of nuclear matrix elements (NMEs) for neutrinoless double-beta decay (0νββ) remains a major theoretical challenge in nuclear physics, as NMEs for this process cannot be accessed directly through experiment. Current nuclear structure models yield significantly different predictions for 0νββ NMEs, making it essential to validate theoretical approaches using observables that are experimentally known. In contrast, two-neutrino double-beta decay (2νββ) has been measured in eleven isotopes, providing a valuable benchmark for testing the reliability of nuclear many-body methods. In this work, we compute the 2νββ decay half-life of 48Ca using the Second Tamm-Dancoff Approximation (STDA) and the Equation of Motion Phonon Method (EMPM). By extending EMPM up to two-phonon configurations, we confirm that the two approaches yield practically identical numerical results, providing a strong internal consistency check. In addition, we study the dependence of the 2νββ NME on the Gamow-Teller and Fermi contributions, on the particle-hole interaction strength parameter gph. Accurately reproducing the experimental 2νββ half-life requires a substantial quenching of the axial-vector coupling constant gA. Furthermore, our theoretical framework outlines a strategy to mitigate this quenching issue by systematically including more complex configurations in the nuclear wave function.

The calculation of nuclear matrix elements (NMEs) for neutrinoless double-beta decay (0νββ) remains a major theoretical challenge in nuclear physics, as NMEs for this process cannot be accessed directly through experiment. Current nuclear structure models yield significantly different predictions for 0νββ NMEs, making it essential to validate theoretical approaches using observables that are experimentally known. In contrast, two-neutrino double-beta decay (2νββ) has been measured in eleven isotopes, providing a valuable benchmark for testing the reliability of nuclear many-body methods. In this work, we compute the 2νββ decay half-life of 48Ca using the Second Tamm-Dancoff Approximation (STDA) and the Equation of Motion Phonon Method (EMPM). By extending EMPM up to two-phonon configurations, we confirm that the two approaches yield practically identical numerical results, providing a strong internal consistency check. In addition, we study the dependence of the 2νββ NME on the Gamow-Teller and Fermi contributions, on the particle-hole interaction strength parameter gph. Accurately reproducing the experimental 2νββ half-life requires a substantial quenching of the axial-vector coupling constant gA. Furthermore, our theoretical framework outlines a strategy to mitigate this quenching issue by systematically including more complex configurations in the nuclear wave function.

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