1988
DOI: 10.1103/physrevd.37.2575
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Neutrinoless double-beta decay with Majoron emission

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1988
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Cited by 38 publications
(34 citation statements)
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“…This limit is almost a factor of 2 more stringent than the previous best limit for this isotope [30]. Taking into account the phase space factors given in [31] and the NME calculated in [16][17][18][19][20], an upper bound on the Majoron-neutrino coupling constant is obtained, hg ee i < ð1.6-3.0Þ × 10 −5 . The limits on lepton number violating parameters obtained here have comparable sensitivity to the best current results obtained with other isotopes, as shown in Table X and in Fig.…”
Section: Search For Neutrinoless Double-β Decaymentioning
confidence: 99%
“…This limit is almost a factor of 2 more stringent than the previous best limit for this isotope [30]. Taking into account the phase space factors given in [31] and the NME calculated in [16][17][18][19][20], an upper bound on the Majoron-neutrino coupling constant is obtained, hg ee i < ð1.6-3.0Þ × 10 −5 . The limits on lepton number violating parameters obtained here have comparable sensitivity to the best current results obtained with other isotopes, as shown in Table X and in Fig.…”
Section: Search For Neutrinoless Double-β Decaymentioning
confidence: 99%
“…happens to be same nucleon recoil operator as appears in Doi et al, [5], except for the sign of the second term. (We believe the sign difference is due to an error in ref.…”
mentioning
confidence: 91%
“…The most promising processes of this type are the lepton-number violating neutrinoless decay (ββ 0ν ), and the decay ββ M , in which the two outgoing electrons are accompanied by a Nambu-Golstone boson, called the majoron. Both processes were predicted [4,5] by the model introduced by Gelmini and Roncadelli [6]. While this simple and elegant model stimulated many experimental searches, it was subsequently found to be incompatible with the LEP measurement of the invisible width of the Z boson [7,8].…”
mentioning
confidence: 99%
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