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Biennial Report 2005-2007 - Saha Institute of Nuclear Physics

Biennial Report 2005-2007 - Saha Institute of Nuclear Physics

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8 <strong>Biennial</strong> <strong>Report</strong> <strong>2005</strong>-071.2.2.6 R-parity violation in NMSSMWe have studied a novel mechanism <strong>of</strong> neutrino mass generation in the Next-to-Minimal supersymmetricmodel. In the Minimal Supersymmetric Standard Model with bilinear R-parity violation,only one neutrino eigenstate acquires a mass at tree level, consequently experimental data on neutrinoscannot be accommodated at tree level. We show that in the Next-to-Minimal extension,where a gauge singlet superfield is added to primarily address the so-called µ-problem, it is possibleto generate two massive neutrino states at tree level. Hence, the global three-flavour neutrinodata can be reproduced at tree level, without appealing to loop dynamics which is vulnerable tomodel-dependent uncertainties. We give analytical expressions for the neutrino mass eigenvaluesand present examples <strong>of</strong> realistic parameter choices.G Bhattacharyya, A Abada†, G Moreau†Theo1.2.2.7 Radiactive neutrino decay and CP violation in R-parity violating SupersymmetryWe have calculated the radiative decay amplitude for Majorana neutrinos in trilinear R-parityviolating supersymmetric framework. Our results make no assumption regarding the masses andmixings <strong>of</strong> fermions and sfermions. The results obtained are exemplary for generic models withloop-generated neutrino masses. Comparison <strong>of</strong> this amplitude with the neutrino mass matrixshows that the two provide independent probes <strong>of</strong> CP-violating phases.G Bhattacharyya, PB Pal, H Päs†, TJ Weiler†Theo1.2.2.8 PDF and scale uncertainties <strong>of</strong> various DY distributions in ADD and RSmodels at hadron collidersIn the extra dimension models <strong>of</strong> ADD and RS we study the dependence <strong>of</strong> the various partondistribution functions on observables <strong>of</strong> DrellYan processes to NLO in QCD at LHC and Tevatronenergies. Uncertainties at LHC due to factorisation scales in going from leading to next-to-leadingorder in QCD for the various distributions get reduced by about 2.75 times for a µ F range 0.5Q< µ F

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