Abstract
The emission of a charged light lepton pair by a superluminal neutrino has been identified as a major factor in the energy loss of highly energetic neutrinos. The observation of PeV neutrinos by IceCube implies their stability against lepton pair Cerenkov radiation. Under the assumption of a Lorentz-violating dispersion relation for highly energetic superluminal neutrinos, one may thus constrain the Lorentz-violating parameters. A kinematically different situation arises when one assumes a Lorentz-covariant, space-like dispersion relation for hypothetical tachyonic neutrinos, as an alternative to Lorentz-violating theories. We here discuss a hitherto neglected decay process, where a highly energetic tachyonic neutrino may emit other (space-like, tachyonic) neutrino pairs. We find that the space-like dispersion relation implies the absence of a q2 threshold for the production of a tachyonic neutrino-antineutrino pair, thus leading to the dominant additional energy loss mechanism for an oncoming tachyonic neutrino in the medium-energy domain. Surprisingly, the small absolute values of the decay rate and energy loss rate in the tachyonic model imply that these models, in contrast to the Lorentz-violating theories, are not pressured by the cosmic PeV neutrinos registered by the IceCube collaboration.
Recommended Citation
U. D. Jentschura and I. Nandori, "Neutrino Pair Cerenkov Radiation for Tachyonic Neutrinos," Advances in High Energy Physics, Hindawi Limited, Nov 2017.
The definitive version is available at https://doi.org/10.1155/2017/9850312
Department(s)
Physics
Keywords and Phrases
Parity; Solitons; Balanced gain
International Standard Serial Number (ISSN)
1687-7357; 1687-7365
Document Type
Article - Journal
Document Version
Final Version
File Type
text
Language(s)
English
Rights
© 2017 Ulrich D. Jentschura and Istvan Nandori, All rights reserved.
Creative Commons Licensing
This work is licensed under a Creative Commons Attribution 4.0 License.
Publication Date
01 Nov 2017
Comments
This research has been supported by the NSF (Grant PHY-1403937) and by a Janos Bolyai Research Scholarship of the Hungarian Academy of Sciences.