SUSY Renormalization Group Effects in Ultra High Energy Neutrinos

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SUSY Renormalization Group Effects in Ultra High Energy Neutrinos. / Bustamante, M.; Gago, A. M.; Jones-Perez, J.

In: Journal of High Energy Physics, Vol. 2011, No. 05, 133, 13.12.2010.

Research output: Contribution to journalJournal articleResearchpeer-review

Harvard

Bustamante, M, Gago, AM & Jones-Perez, J 2010, 'SUSY Renormalization Group Effects in Ultra High Energy Neutrinos', Journal of High Energy Physics, vol. 2011, no. 05, 133. https://doi.org/10.1007/JHEP05(2011)133

APA

Bustamante, M., Gago, A. M., & Jones-Perez, J. (2010). SUSY Renormalization Group Effects in Ultra High Energy Neutrinos. Journal of High Energy Physics, 2011(05), [133]. https://doi.org/10.1007/JHEP05(2011)133

Vancouver

Bustamante M, Gago AM, Jones-Perez J. SUSY Renormalization Group Effects in Ultra High Energy Neutrinos. Journal of High Energy Physics. 2010 Dec 13;2011(05). 133. https://doi.org/10.1007/JHEP05(2011)133

Author

Bustamante, M. ; Gago, A. M. ; Jones-Perez, J. / SUSY Renormalization Group Effects in Ultra High Energy Neutrinos. In: Journal of High Energy Physics. 2010 ; Vol. 2011, No. 05.

Bibtex

@article{5491771cdb2443c6b46c4cc61ff9cc56,
title = "SUSY Renormalization Group Effects in Ultra High Energy Neutrinos",
abstract = "We have explored the question of whether the renormalization group running of the neutrino mixing parameters in the Minimal Supersymmetric Standard Model is detectable with ultra-high energy neutrinos from active galactic nuclei (AGN). We use as observables the ratios of neutrino fluxes produced at the AGN, focusing on four different neutrino production models: $(\Phi_{\nu_e+\bar{\nu}_e}^0 : \Phi_{\nu_\mu+\bar{\nu}_\mu}^0 : \Phi_{\nu_\tau+\bar{\nu}_\tau}^0)$ = (1:2:0), (0:1:0), (1:0:0), and (1:1:0). The prospects for observing deviations experimentally are taken into consideration, and we find out that it is necessary to impose a cut-off on the transferred momentum of $Q^2 \geq 10^7$ GeV$^2$. However, this condition, together with the expected low value of the diffuse AGN neutrino flux, yields a negligible event rate at a km-scale Cherenkov detector such as IceCube.",
keywords = "hep-ph, astro-ph.HE",
author = "M. Bustamante and Gago, {A. M.} and J. Jones-Perez",
note = "26 pages, 9 figures. Version accepted for publication in JHEP",
year = "2010",
month = dec,
day = "13",
doi = "10.1007/JHEP05(2011)133",
language = "English",
volume = "2011",
journal = "Journal of High Energy Physics (Online)",
issn = "1126-6708",
publisher = "Springer",
number = "05",

}

RIS

TY - JOUR

T1 - SUSY Renormalization Group Effects in Ultra High Energy Neutrinos

AU - Bustamante, M.

AU - Gago, A. M.

AU - Jones-Perez, J.

N1 - 26 pages, 9 figures. Version accepted for publication in JHEP

PY - 2010/12/13

Y1 - 2010/12/13

N2 - We have explored the question of whether the renormalization group running of the neutrino mixing parameters in the Minimal Supersymmetric Standard Model is detectable with ultra-high energy neutrinos from active galactic nuclei (AGN). We use as observables the ratios of neutrino fluxes produced at the AGN, focusing on four different neutrino production models: $(\Phi_{\nu_e+\bar{\nu}_e}^0 : \Phi_{\nu_\mu+\bar{\nu}_\mu}^0 : \Phi_{\nu_\tau+\bar{\nu}_\tau}^0)$ = (1:2:0), (0:1:0), (1:0:0), and (1:1:0). The prospects for observing deviations experimentally are taken into consideration, and we find out that it is necessary to impose a cut-off on the transferred momentum of $Q^2 \geq 10^7$ GeV$^2$. However, this condition, together with the expected low value of the diffuse AGN neutrino flux, yields a negligible event rate at a km-scale Cherenkov detector such as IceCube.

AB - We have explored the question of whether the renormalization group running of the neutrino mixing parameters in the Minimal Supersymmetric Standard Model is detectable with ultra-high energy neutrinos from active galactic nuclei (AGN). We use as observables the ratios of neutrino fluxes produced at the AGN, focusing on four different neutrino production models: $(\Phi_{\nu_e+\bar{\nu}_e}^0 : \Phi_{\nu_\mu+\bar{\nu}_\mu}^0 : \Phi_{\nu_\tau+\bar{\nu}_\tau}^0)$ = (1:2:0), (0:1:0), (1:0:0), and (1:1:0). The prospects for observing deviations experimentally are taken into consideration, and we find out that it is necessary to impose a cut-off on the transferred momentum of $Q^2 \geq 10^7$ GeV$^2$. However, this condition, together with the expected low value of the diffuse AGN neutrino flux, yields a negligible event rate at a km-scale Cherenkov detector such as IceCube.

KW - hep-ph

KW - astro-ph.HE

U2 - 10.1007/JHEP05(2011)133

DO - 10.1007/JHEP05(2011)133

M3 - Journal article

VL - 2011

JO - Journal of High Energy Physics (Online)

JF - Journal of High Energy Physics (Online)

SN - 1126-6708

IS - 05

M1 - 133

ER -

ID: 184744872