TY - JOUR
T1 - Neutrino mass matrix in the minimal supergravity model
T2 - Bi-large mixing with trilinear R-parity violation
AU - Chun, Eung Jin
AU - Jung, Dong Won
AU - Kang, Sin Kyu
AU - Park, Jong Dac
PY - 2004/11
Y1 - 2004/11
N2 - We study the neutrino oscillation and the production/decay of the lightest supersymmetric particle (LSP) under the minimal supergravity model (mSUGRA) without R-parity. The supersymmetric model without R-parity can explain the neutrino masses and mixing naturally, and has the virtue that it can be probed by collidcr experiments, by observing the decay of the LSP. In this paper, we show that we can describe the neutrino masses and mixing well under the mSUGRA without R-parity. In general, the 1-loop corrections are important to explain the known structure of neutrino oscillation. In mSUGRA, the neutraliho is LSP in most cases, but there is a small region which makes the scalar tau LSP. We search that region. For each case, we calculate the decay rate and branching ratios; as a result, we can find that it is possible to allow or exclude the model in the small tan β region. Unfortunately, it is impossible to probe the model in the large tan/3 case, because of the interferences among some diagrams of the LSP decay.
AB - We study the neutrino oscillation and the production/decay of the lightest supersymmetric particle (LSP) under the minimal supergravity model (mSUGRA) without R-parity. The supersymmetric model without R-parity can explain the neutrino masses and mixing naturally, and has the virtue that it can be probed by collidcr experiments, by observing the decay of the LSP. In this paper, we show that we can describe the neutrino masses and mixing well under the mSUGRA without R-parity. In general, the 1-loop corrections are important to explain the known structure of neutrino oscillation. In mSUGRA, the neutraliho is LSP in most cases, but there is a small region which makes the scalar tau LSP. We search that region. For each case, we calculate the decay rate and branching ratios; as a result, we can find that it is possible to allow or exclude the model in the small tan β region. Unfortunately, it is impossible to probe the model in the large tan/3 case, because of the interferences among some diagrams of the LSP decay.
KW - Collider signatures
KW - Neutrino mass and mixing
KW - R-parity violation
UR - https://www.scopus.com/pages/publications/19744367675
M3 - Article
AN - SCOPUS:19744367675
SN - 0374-4884
VL - 45
SP - S278-S284
JO - Journal of the Korean Physical Society
JF - Journal of the Korean Physical Society
IS - 2 SUPPL.
ER -