35 research outputs found

    Drell-Yan, ZZ, W+W- production in SM & ADD model to NLO+PS accuracy at the LHC

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    In this paper, we present the next-to-leading order QCD corrections for di-lepton, di-electroweak boson (ZZ, W+W-) production in both the SM and the ADD model, matched to the HERWIG parton-shower using the aMC@NLO framework. A selection of results at the 8 TeV LHC, which exhibits deviation from the SM as a result of the large extra-dimension scenario are presented.Comment: 12 pages, 10 figures, search sensitivity for the 14 TeV LHC discussed, version to appear in Eur. Phys. J.

    Vector boson production in association with KK modes of the ADD model to NLO in QCD at LHC

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    Next-to-leading order QCD corrections to the associated production of vector boson (Z/W) with the the Kaluza-Klein modes of the graviton in large extra dimensional model at the LHC, are presented. We have obtained various kinematic distributions using a Monte Carlo code which is based on the two cut off phase space slicing method that handles soft and collinear singularities appearing at NLO level. We estimate the impact of the QCD corrections on various observables and find that they are significant. We also show the reduction in factorization scale uncertainty when QCD corrections are included.Comment: 12 pages, 5 figure

    Di-jet production at the LHC through unparticles

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    We report the phenomenological impact of unparticles in the production of di-jet at the LHC. We compute the scalar, spin-1 and spin-2 unparticle contributions to the dijet cross sections and present our results in different kinematical distributions. We find that the scalar unparticle contribution is dominant over that of the spin-1 and spin-2 unparticles for the same coupling values.Comment: 17 pages, 10 eps figures, 4 tables. Spin-1 unparticles also included. This version to appear in PR

    NLO-QCD corrections to e+ e- --> hadrons in models of TeV-scale gravity

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    We present results on NLO-QCD corrections to the process e+ e- --> hadrons via photon-, Z- and graviton-exchange in the context of TeV-scale gravity models. The quantitative impact of these QCD corrections for searches of extra dimensions at a Linear Collider is briefly discussed.Comment: 10 pages, LaTeX, using axodraw.st

    PDF and scale uncertainties of various DY distributions in ADD and RS models at hadron colliders

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    In the extra dimension models of ADD and RS we study the dependence of the various parton distribution functions on observable of Drell-Yan process to NLO in QCD at LHC and Tevatron energies. Uncertainties at LHC due to factorisation scales in going from leading to next-to-leading order in QCD for the various distributions get reduced by about 2.75 times for a μF\mu_F range 0.5 Q<μF<1.5 Q0.5 ~Q < \mu_F < 1.5 ~Q. Further uncertainties arising from the error on experimental data are estimated using the MRST parton distribution functions.Comment: 27 pages, 11 figures, the version to appear in European Physical Journal

    Constraints on Astro-unparticle Physics from SN 1987A

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    SN 1987A observations have been used to place constraints on the interactions between standard model particles and unparticles. In this study we calculate the energy loss from the supernovae core through scalar, pseudo scalar, vector, pseudo vector unparticle emission from nuclear bremsstrahlung for degenerate nuclear matter interacting through one pion exchange. In order to examine the constraints on dU=1d_{\cal U}=1 we considered the emission of scalar, pseudo scalar, vector, pseudo vector and tensor through the pair annihilation process e+eUγe^+e^-\to {\cal U} \gamma . In addition we have re-examined other pair annihilation processes. The most stringent bounds on the dimensionless coupling constants for dU=1d_{\cal U} =1 and ΛU=mZ\Lambda_{\cal U}= m_Z are obtained from nuclear bremsstrahlung process for the pseudo scalar and pseudo-vector couplings λ0,1P4×1011\bigl|\lambda^{\cal P}_{0,1}\bigr|\leq 4\times 10^{-11} and for tensor interaction, the best limit on dimensionless coupling is obtained from e+eUγe^+ e^-\to {\cal U} \gamma and we get λT6×106\bigl|\lambda^{\cal T}\bigr| \leq 6\times 10^{-6}.Comment: 12 pages, 2 postscript figure

    Constraints from Solar and Reactor Neutrinos on Unparticle Long-Range Forces

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    We have investigated the impact of long-range forces induced by unparticle operators of scalar, vector and tensor nature coupled to fermions in the interpretation of solar neutrinos and KamLAND data. If the unparticle couplings to the neutrinos are mildly non-universal, such long-range forces will not factorize out in the neutrino flavour evolution. As a consequence large deviations from the observed standard matter-induced oscillation pattern for solar neutrinos would be generated. In this case, severe limits can be set on the infrared fix point scale, Lambda_u, and the new physics scale, M, as a function of the ultraviolet (d_UV) and anomalous (d) dimension of the unparticle operator. For a scalar unparticle, for instance, assuming the non-universality of the lepton couplings to unparticles to be of the order of a few per mil we find that, for d_UV=3 and d=1.1, M is constrained to be M > O(10^9) TeV (M > O(10^10) TeV) if Lambda_u= 1 TeV (10 TeV). For given values of Lambda_u and d, the corresponding bounds on M for vector [tensor] unparticles are approximately 100 [3/Sqrt(Lambda_u/TeV)] times those for the scalar case. Conversely, these results can be translated into severe constraints on universality violation of the fermion couplings to unparticle operators with scales which can be accessible at future colliders.Comment: 13 pages, 3 figures. Minor changes due to precision in numerical factors and correction in figure labels. References added. Conclusions remain unchange
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