Abstract

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 λ1,2,3 \lambda'_{1,2,3} and λ1,2\lambda_{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 λ1<λ2λ3| \lambda'_1 | < | \lambda'_2| \sim | \lambda'_3|, and λ1λ2|\lambda_1| \sim |\lambda_2| are required by the large atmospheric neutrino mixing angle θ23\theta_{23} and the small angle θ13\theta_{13}, and the large solar neutrino mixing angle θ12\theta_{12}, 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 λ12:λ22:λ12+λ22|\lambda_1|^2: |\lambda_2|^2: |\lambda_1|^2 + |\lambda_2|^2 can be measured by establishing Br(eν):Br(μν):Br(τν)Br(e\nu): Br(\mu\nu) : Br(\tau\nu) or Br(νe±τ):Br(νμ±τ):Br(ντ±τ)Br(\nu e^\pm \tau^\mp ): Br(\nu\mu^\pm\tau^\mp) : Br(\nu\tau^\pm\tau^\mp), respectively. The information on the couplings λi\lambda'_i can be drawn by measuring Br(litbˉ)λi2Br(l_i t \bar{b}) \propto |\lambda'_i|^2 if the neutralino LSP is heavier than the top quark.Comment: RevTex, 25 pages, 8 eps figure

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    Last time updated on 01/04/2019