Abstract
The Operator Expansion Method (OEM) for the calculation of two-neutrino double beta decay (2ν2β-decay) is reconsidered. The assumed two-body Hamiltonian, in contrast to the ones considered previously, allows a consistent derivation of the OEM transition operators. The OEM is combined with the renormalized proton-neutron QRPA (pn-RQRPA) ground state wave functions and the 2ν2β-decay of76Ge is calculated. The influence and relative importance of the central, tensor and Coulomb interactions are investigated. We have found that the strong suppression of the nuclear matrix elementM GT has its origin in the choice of the pn-RQRPA ground state wave functions of the initial and final nuclei.
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Simkovic, F., Veselský, M. Dooble beta decay: Operator expasion method revisited. Czech J Phys 48, 245–248 (1998). https://doi.org/10.1023/A:1021284412852
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DOI: https://doi.org/10.1023/A:1021284412852