1966
DOI: 10.1103/physrev.146.810
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Limits for Lepton-Conserving and Lepton-Nonconserving Double Beta Decay inCa48

Abstract: quadrupole angular distributions although we are not in disagreement with the 1=4 contributions, predicted by the shell model. 24 In addition, the sum of their differential cross sections equals that of the first 2+ in Cr 52 . As seen in Table III their B(E2)[ values are not equal to the Cr 52 state.It is interesting to note that the sum rule predicted by the weak-coupling model 25 holds even though the 24 H. O. Fimston, N. R. Robertson, and E. Rost, Phys. Rev. 134, B117 (1964). 25 A. de-Shalit, Phys. Rev. 1… Show more

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Cited by 58 publications
(22 citation statements)
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“…Searches for the 0νββ decay of 48 Ca began 60 years ago [25]. The main experimental technique that has been employed is the use of scintillating CaF 2 crystals [26][27][28]. Such detectors have good energy resolution and detection efficiency in order to search for a line at Q ββ , while backgrounds generally prevent a straightforward measurement of the 2νββ rate.…”
Section: Introductionmentioning
confidence: 99%
“…Searches for the 0νββ decay of 48 Ca began 60 years ago [25]. The main experimental technique that has been employed is the use of scintillating CaF 2 crystals [26][27][28]. Such detectors have good energy resolution and detection efficiency in order to search for a line at Q ββ , while backgrounds generally prevent a straightforward measurement of the 2νββ rate.…”
Section: Introductionmentioning
confidence: 99%
“…It is worth to mention a pioneering work of der Mateosian and Goldhaber to search for neutrinoless decay of by using enriched and depleted in ( and ) crystal scintillators [25]. Several high sensitivity studies of processes were realized using crystal scintillators, which contain candidate nuclei (see Table I).…”
Section: Scintillators In Experimentsmentioning
confidence: 99%
“…1c Hence, we conclude that "active" source approach provides 4π geometry for the source, absence of self-absorption, and better energy resolution, which does not depend on the angular and energy distribution of the electrons emitted in 2β decay. These advantages of "active" detectors were understood a long ago and the first experiment of this type was performed in 1966 by using 48 CaF 2 scintillator to study 2β decay of 48 Ca [23]. In the next year semiconductor Ge(Li) crystal was applied in the quest for 2β decay of 76 Ge [24].…”
Section: Introductionmentioning
confidence: 99%