中文

Double beta decay transition mechanism

核理论 2016-08-14 v1

摘要

After briefly reviewing ββ\beta \beta decay as a test of the neutrino mass, I examine the nuclear structure involved in this process. Simple formulas (\`{a} la Pad\'{e}) are designed for the transition amplitudes and the general behavior of ββ\beta \beta decay amplitudes in the quasiparticle random phase approximation are discussed. Results of a calculation for 48Ca^{48}Ca, 76Ge^{76}Ge , 82Se^{82}Se, 100Mo^{100}Mo, 128Te^{128}Te and 130Te^{130}Te nuclei are presented, in which the particle-particle interaction strengths have been fixed by invoking the partial restoration of the isospin and Wigner SU(4) symmetries. An upper limit of <mν>1 <m_{\nu}>\approx 1 eV is obtained for the effective neutrino mass.

关键词

引用

@article{arxiv.nucl-th/9403018,
  title  = {Double beta decay transition mechanism},
  author = {F. Krmpotić},
  journal= {arXiv preprint arXiv:nucl-th/9403018},
  year   = {2016}
}

备注

LaTeX and 5 figures, talk given at the `XVII Symposium on Nuclear Physics', Oaxtepec, Mexico, 4-7 January 1994. LaTeX source modified by arXiv admin so that paper compiles in spite of omitted definition file. See source for details