Majoron
Bosonic | |
|---|---|
| Family | Goldstone Boson |
| Status | Hypothetical |
| Symbol | J |
| Theorized | Y. Chikashige, R. N. Mohapatra, and R. D. Peccei |
| Mass | unknown |
| Electric charge | 0 e |
| Spin | 0[1] |
In
B − L
in certain high energy collisions such as
- +
W−
J
Where two
spatial dimensions the detectable number of majoron creation events vary accordingly. Mathematically, majorons may be modeled by allowing them to propagate through a material while all other Standard Model forces are fixed to an orbifold
point.
Searches
Experiments studying double beta decay have set limits on decay modes that emit majorons.
.References
Further reading
- Balysh, A.; et al. (1996). "Bounds on new Majoron models from the Heidelberg-Moscow experiment". S2CID 31618565.
- Mohapatra, R.N.; Pérez-Lorenzana, A.; de S. Pires, C.A. (2000). "Neutrino mass, bulk majoron and neutrinoless double beta decay". Physics Letters B. 491 (1–2): 143–147. S2CID 119527305.
- Carone, C.D.; Conroy, J.M.; Kwee, H.J. (2002). "Bulk majorons at colliders". S2CID 119099210.
- Frampton, P.H.; Oh, M.C.; Yoshikawa, T. (2002). "Majoron mass zeros from Higgs triplet vacuum expectation values without a Majoron problem". S2CID 119358575.
- Grossman, Y.; Haber, H.E. (2003). "The would-be Majoron in R-parity-violating supersymmetry". S2CID 35069267.
- de S. Pires, C.A.; Rodrigues da Silva, P.S. (2004). "Spontaneous breaking of the lepton number and invisible majoron in a 3-3-1 model". S2CID 195317240.
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