2013
DOI: 10.1002/andp.201200222
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Status and prospects of searches for neutrinoless double beta decay

Abstract: Abstract. The simultaneous beta decay of two neutrons in a nucleus without the emission of neutrinos (called neutrinoless double beta decay) is a lepton number violating process which is not allowed in the Standard Model of particle physics. More than a dozen experiments using different candidate isotopes and a variety of detection techniques are searching for this decay. Some (EXO-200, Kamland-Zen, GERDA) started to take data recently. EXO and KamlandZen have reported first limits of the half life T

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Cited by 84 publications
(79 citation statements)
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References 84 publications
(116 reference statements)
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“…(5), G is the (calculable) phase space and M is the nuclear matrix element (NME) for a candidate nucleus [15,[50][51][52]. A worldwide search is underway to find possible 0νββ decay signatures in a variety of nuclei, and lower limits on the corresponding half lives have been placed [53][54][55]. Transforming lower bounds on T into upper bounds on m ββ requires theoretical input on the NME and their uncertainties [15,[50][51][52][56][57][58].…”
Section: B Neutrinoless Double Beta Decaymentioning
confidence: 99%
See 1 more Smart Citation
“…(5), G is the (calculable) phase space and M is the nuclear matrix element (NME) for a candidate nucleus [15,[50][51][52]. A worldwide search is underway to find possible 0νββ decay signatures in a variety of nuclei, and lower limits on the corresponding half lives have been placed [53][54][55]. Transforming lower bounds on T into upper bounds on m ββ requires theoretical input on the NME and their uncertainties [15,[50][51][52][56][57][58].…”
Section: B Neutrinoless Double Beta Decaymentioning
confidence: 99%
“…9 (dominated by cosmology). There are good prospects to further probe this region -and possibly go below it-with upcoming or planned 0νββ experiments [53][54][55]. However, unlike Σ, there is no finite lower bound on m ββ , since the null value cannot be excluded a priori for unfavorable Majorana phases (see [102] and refs.…”
Section: Combined Constraints In the (σ M ββ ) Planementioning
confidence: 99%
“…We are particularly interested to determine accurately the conditions for which |m ββ | 0.01 eV, which may be probed experimentally in the near future (see refs. [36][37][38][39][40][41]), and the conditions for which there can be a cancellation of the different mass contributions to |m ββ |, which leads to an unfortunate uncertainty for the possibility of ever observing neutrinoless double-beta decay (unless it is induced by new interactions and/or the exchange of new particles; see refs. [42][43][44][45][46][47][48][49]).…”
Section: Jhep07(2015)171mentioning
confidence: 99%
“…At least a part of the second region is accessible to the next generation of neutrinoless double-beta decay experiments (see refs. [36][37][38][39][40][41]). The only β-decay experiment under preparation with the aim of exploring the sub-eV region of m β is KATRIN [98], which will have a sensitivity of about 0.2 eV that is not sufficient to explore the upper part of the region in figure 15 allowed only in the case of 3+1 mixing.…”
Section: Jhep07(2015)171mentioning
confidence: 99%
“…This is, however, in conflict with the most stringent upper limit on the sum of light neutrino masses, i m i < 0.23 eV at 95% confidence level (CL), obtained from Planck data [7]. Hence, any evidence of a positive signal in the upcoming 0νββ experiments [8], 1 could indicate a new physics contribution to this rare LNV process.…”
Section: Introductionmentioning
confidence: 91%