TY - JOUR
T1 - Neutrino oscillations and collider test of the R-parity violating minimal supergravity model
AU - Jung, Dong Won
AU - Kang, Sin Kyu
AU - Park, Jong Dae
AU - Chun, Eung Jin
PY - 2004/8/1
Y1 - 2004/8/1
N2 - We study the R-parity violating minimal supergravity models accounting for the observed neutrino masses and mixing, which can be tested in future collider experiments. The bi-large mixing can be explained by allowing five dominant tri-linear couplings λ′1,2,3 and λ′ 1,2. The desired ratio of the atmospheric and solar neutrino mass-squared differences can be obtained in a very limited parameter space where the tree-level contribution is tuned to be suppressed. In this allowed region, we quantify the correlation between the three neutrino mixing angles and the tri-linear R-parity violating couplings. Qualitatively, the relations λ′1| < |λ′2 ∼ |λ′3, and |λ1| ∼ |λ2 are required by the large atmospheric neutrino mixing angle θ23 and the small angle θ13, and the large solar neutrino mixing angle θ12, respectively. Such a prediction on the couplings can be tested in the next linear colliders by observing the branching ratios of the lightest supersymmetric particle (LSP). For the stau or the neutralino LSP, the ratio |λ1|2 : |λ2 |2 : |λ1 |2 + |λ2 |2 can be measured by establishing Br(ev) : Br(μv) : Br(τv) or Br(ve±τ∓) : Br(vμ±τ∓) : Br(vτ ±τ∓), respectively. The information on the couplings λ′i can be drawn by measuring Br(l itb̄) α |λ′i|2 if the neutralino LSP is heavier than the top quark.
AB - We study the R-parity violating minimal supergravity models accounting for the observed neutrino masses and mixing, which can be tested in future collider experiments. The bi-large mixing can be explained by allowing five dominant tri-linear couplings λ′1,2,3 and λ′ 1,2. The desired ratio of the atmospheric and solar neutrino mass-squared differences can be obtained in a very limited parameter space where the tree-level contribution is tuned to be suppressed. In this allowed region, we quantify the correlation between the three neutrino mixing angles and the tri-linear R-parity violating couplings. Qualitatively, the relations λ′1| < |λ′2 ∼ |λ′3, and |λ1| ∼ |λ2 are required by the large atmospheric neutrino mixing angle θ23 and the small angle θ13, and the large solar neutrino mixing angle θ12, respectively. Such a prediction on the couplings can be tested in the next linear colliders by observing the branching ratios of the lightest supersymmetric particle (LSP). For the stau or the neutralino LSP, the ratio |λ1|2 : |λ2 |2 : |λ1 |2 + |λ2 |2 can be measured by establishing Br(ev) : Br(μv) : Br(τv) or Br(ve±τ∓) : Br(vμ±τ∓) : Br(vτ ±τ∓), respectively. The information on the couplings λ′i can be drawn by measuring Br(l itb̄) α |λ′i|2 if the neutralino LSP is heavier than the top quark.
KW - Neutrino Physics
KW - Supergravity Models
KW - Supersymmetry Phenomenology
UR - http://www.scopus.com/inward/record.url?scp=23044437120&partnerID=8YFLogxK
U2 - 10.1088/1126-6708/2004/08/017
DO - 10.1088/1126-6708/2004/08/017
M3 - Article
AN - SCOPUS:23044437120
SN - 1126-6708
VL - 8
SP - 483
EP - 511
JO - Journal of High Energy Physics
JF - Journal of High Energy Physics
IS - 8
ER -