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Biennial Report 2005-2007 - Saha Institute of Nuclear Physics

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Theoretical <strong>Physics</strong> 9LHC and Tevatron. Inclusion <strong>of</strong> QCD corrections to NLO stabilises the cross section with respectto scale variations.Prakash Mathews, V Ravindran†Theo1.2.2.10 NLO-QCD corrections to dilepton production in the Randall-SundrummodelThe dilepton production process at hadron colliders in the Randall-Sundrum (RS) model is studiedat next-to-leading order in QCD. The NLO-QCD corrections have been computed for the virtualgraviton exchange process in the RS model, in addition to the usual Z-mediated processes <strong>of</strong>standard Drell-Yan. K-factors for the cross-sections at the LHC and Tevatron for differential inthe invariant mass, Q, and the rapidity, Y, <strong>of</strong> the lepton pair are presented. We find the K-factorsare large over substantial regions <strong>of</strong> the phase space.Prakash Mathews, V Ravindran†, K Sridhar†Theo1.2.2.11 Next-to-leading order QCD corrections to the Drell-Yan cross section inmodels <strong>of</strong> TeV-scale gravityThe first results on next-to-leading order QCD corrections to graviton-induced processes in hadroncollisions in models <strong>of</strong> TeV-scale gravity are presented focusing on the case <strong>of</strong> dilepton pair productionand pp collisions. Distributions in the invariant mass Q, the longitudinal fraction x F , therapidity Y and the forward-backward asymmetry <strong>of</strong> the lepton pair are studied. The quantitativeimpact <strong>of</strong> the QCD corrections for searches <strong>of</strong> extra dimensions at hadron colliders is investigated.It turns out that at the LHC the K-factor is rather large (K = 1.6) for large invariant mass Q <strong>of</strong> thelepton pair, indicating the importance <strong>of</strong> accounting for these QCD corrections in the experimentalsearch for TeV-scale gravity. At the Tevatron, the K-factor does not substantially deviate from theStandard Model value. However, its inclusion is necessitated to make the cross section stable withrespect to scale variations.Prakash Mathews, V Ravindran†, K Sridhar†, WL van Neerven†Theo1.2.3 Astrophysics & Cosmology1.2.3.1 Hyperon bulk viscosity and its influence on r-modes <strong>of</strong> neutron starsWe studied the effect <strong>of</strong> hyperon matter on bulk viscosity. In this connection, we have constructedequations <strong>of</strong> state within the framework <strong>of</strong> a relativistic field theoretical model. As large number<strong>of</strong> hyperons may be produced in dense matter, hyperon-hyperon interaction becomes importantand have been included in our calculation. We computed the bulk viscosity coefficient due to thenon-leptonic weak process n + p ⇀↽ p + Λ. It was found that the gravitational radiation drivenr-mode instability was suppressed due to large hyperon bulk viscosity coefficient.Debarati Chatterjee, Debades BandyopadhyayTheo

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