2,284 research outputs found

    One-loop corrections to five-parton amplitudes with external photons

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    Recently the calculations of all five-parton one-loop QCD amplitudes have been completed. In this letter we describe how to get the corresponding amplitudes with one gluon replaced by a photon and we give the explicit results for the process 0 \to 2q 2Q 1\y.Comment: 7 pages, late

    γ5\gamma_{5} in FDH

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    We investigate the regularization-scheme dependent treatment of γ5\gamma_{5} in the framework of dimensional regularization, mainly focusing on the four-dimensional helicity scheme (FDH). Evaluating distinctive examples, we find that for one-loop calculations, the recently proposed four-dimensional formulation (FDF) of the FDH scheme constitutes a viable and efficient alternative compared to more traditional approaches. In addition, we extend the considerations to the two-loop level and compute the pseudo-scalar form factors of quarks and gluons in FDH. We provide the necessary operator renormalization and discuss at a practical level how the complexity of intermediate calculational steps can be reduced in an efficient way.Comment: 28 pages, 7 figure

    Lepton-flavour violating decays in theories with dimension 6 operators

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    Despite a large experimental effort, so far no evidence for flavour-violating decays of charged leptons such as li→ljγl_i\to l_j\gamma and li→ljlklkl_i\to l_j l_k l_k has been found. The absence of a signal puts very severe constraints on many extensions of the Standard Model. Here we apply a model independent approach by studying such decays in the Standard Model effective field theory. Going beyond leading order in the Standard Model couplings and considering all dimension 6 operators that might lead to lepton-flavour violation, we are able to extract limits on a large number of Wilson coefficients of such operators. We are also able to compare the impact of particular searches and find, for example, that flavour-violating decays of the ZZ-boson Z→μeZ\to \mu e are much more constrained from low-energy experiments μ→eγ\mu\to e \gamma than from the limits of current and future direct searches at high energy.Comment: 7 pages, 5 Tables; to appear in the Proceedings of the FCCP2015 Worksho

    Resonant particle production at hadron colliders

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    We present a method to compute off-shell effects for processes involving resonant particles at hadron colliders with the possibility to include realistic cuts on the decay products. The method is based on an effective theory approach to unstable particle production and, as an example, is applied to t-channel single top production at the LHC.Comment: 6 pages, to appear in the proceedings of the 9th International Symposium on Radiative Corrections (RADCOR 2009), October 25-30 2009, Ascona, Switzerlan

    Two-loop Correction to the Leptonic Decay of Quarkonium

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    Applying asymptotic expansions at threshold, we compute the two-loop QCD correction to the short-distance coefficient that governs the leptonic decay ψ→l+l−\psi\to l^+ l^- of a S-wave quarkonium state and discuss its impact on the relation between the quarkonium non-relativistic wave function at the origin and the quarkonium decay constant in full QCD.Comment: 7 pages, LaTeX, 1 figure included via epsf.st

    Fully differential NLO predictions for the radiative decay of muons and taus

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    We present a general purpose Monte Carlo program for the calculation of the radiative muon decay μ→e ννˉγ\mu\to e\,\nu \bar{\nu}\gamma and the radiative decays τ→e ννˉγ\tau\to e\, \nu \bar{\nu}\gamma and τ→μ ννˉγ\tau\to\mu\,\nu \bar{\nu}\gamma at next-to-leading order in the Fermi theory. The full dependence on the lepton masses and polarization of the initial-sate lepton are kept. We study the branching ratios for these processes and show that fully-differential next-to-leading order corrections are important for addressing a tension between BaBar's recent measurement of the branching ratio B(τ→e ννˉγ)\mathcal{B}(\tau\to e\, \nu\bar{\nu}\gamma) and the Standard Model prediction. In addition, we study various distributions of the process μ→e ννˉγ\mu\to e\,\nu \bar{\nu}\gamma and obtain precise predictions for the irreducible background to μ→eγ\mu\to e \gamma searches, tailored to the geometry of the MEG detector.Comment: 14 pages, 5 figures, published versio

    Renormalization-group improved fully differential cross sections for top pair production

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    We extend approximate next-to-next-to-leading order results for top-pair production to include the semi-leptonic decays of top quarks in the narrow-width approximation. The new hard-scattering kernels are implemented in a fully differential parton-level Monte Carlo that allows for the study of any IR-safe observable constructed from the momenta of the decay products of the top. Our best predictions are given by approximate NNLO corrections in the production matched to a fixed order calculation with NLO corrections in both the production and decay subprocesses. Being fully differential enables us to make comparisons between approximate results derived via different (PIM and 1PI) kinematics for arbitrary distributions. These comparisons reveal that the renormalization-group framework, from which the approximate results are derived, is rather robust in the sense that applying a realistic error estimate allows us to obtain a reliable prediction with a reduced theoretical error for generic observables and analysis cuts

    Performance tests with a 4.75 inch bore tapered-roller bearings at high speeds

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    The tapered-roller bearings were tested at speeds to 15,000 rpm which results in a cone-rib tangential velocity of 130 m/sec. (25,500 ft/min). Lubrication was applied either by jets or directly to the cone-rib, augmented with jets. Additional test parameters included thrust loads to 53,400 N (12,000 lbs), radial loads to 26,700 N (6,000 lbs), lubricant flow rates from 1.9 x 0.000 to 15.1 x 0.001 cubic meter/min. (0.5 to 4.0 gpm), and lubricant inlet temperatures of 350 K and 364 K (170 F and 195 F). Temperature distribution, separator speed, and drive-motor power demand were determined as functions of these test parameters
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