Soft-gluon resummation for squark and gluino hadroproduction

We consider the resummation of soft gluon emission for squark and gluino hadroproduction at next-to-leading-logarithmic (NLL) accuracy in the framework of the minimal supersymmetric standard model. We present analytical results for squark-squark and squark-gluino production and provide numerical predictions for all squark and gluino pair-production processes at the Tevatron and at the LHC. The size of the soft-gluon corrections and the reduction in the scale uncertainty are most significant for processes involving gluino production. At the LHC, where the sensitivity to squark and gluino masses ranges up to 3 TeV, the corrections due to NLL resummation over and above the NLO predictions can be as high as 35% in the case of gluino-pair production, whereas at the Tevatron, the NLL corrections are close to 40% for squark-gluino final states with sparticle masses around 500 GeV.Comment: 31 pages, 7 figure

Implementation of electroweak corrections in the POWHEG BOX: single W production

We present a fully consistent implementation of electroweak and strong radiative corrections to single W hadroproduction in the POWHEG BOX framework, treating soft and collinear photon emissions on the same ground as coloured parton emissions. This framework can be easily extended to more complex electroweak processes. We describe how next-to-leading order (NLO) electroweak corrections are combined with the NLO QCD calculation, and show how they are interfaced to QCD and QED shower Monte Carlo. The resulting tool fills a gap in the literature and allows to study comprehensively the interplay of QCD and electroweak effects to W production using a single computational framework. Numerical comparisons with the predictions of the electroweak generator HORACE, as well as with existing results on the combination of electroweak and QCD corrections to W production, are shown for the LHC energies, to validate the reliability and accuracy of the approachComment: 31 pages, 7 figures. Minor corrections, references added and updated. Final version to appear in JHE

Combination of electroweak and QCD corrections to single W production at the Fermilab Tevatron and the CERN LHC

Precision studies of the production of a high-transverse momentum lepton in association with missing energy at hadron colliders require that electroweak and QCD higher-order contributions are simultaneously taken into account in theoretical predictions and data analysis. Here we present a detailed phenomenological study of the impact of electroweak and strong contributions, as well as of their combination, to all the observables relevant for the various facets of the p\smartpap \to {\rm lepton} + X physics programme at hadron colliders, including luminosity monitoring and Parton Distribution Functions constraint, $W$ precision physics and search for new physics signals. We provide a theoretical recipe to carefully combine electroweak and strong corrections, that are mandatory in view of the challenging experimental accuracy already reached at the Fermilab Tevatron and aimed at the CERN LHC, and discuss the uncertainty inherent the combination. We conclude that the theoretical accuracy of our calculation can be conservatively estimated to be about 2% for standard event selections at the Tevatron and the LHC, and about 5% in the very high $W$ transverse mass/lepton transverse momentum tails. We also provide arguments for a more aggressive error estimate (about 1% and 3%, respectively) and conclude that in order to attain a one per cent accuracy: 1) exact mixed ${\cal O}(\alpha \alpha_s)$ corrections should be computed in addition to the already available NNLO QCD contributions and two-loop electroweak Sudakov logarithms; 2) QCD and electroweak corrections should be coherently included into a single event generator.Comment: One reference added. Final version to appear in JHE

SUSY QCD corrections to electroweak gauge boson production with an associated jet at the LHC

We study the stability of the neutral- and charged-current Drell-Yan process in association with a jet as a standard candle at the LHC under the inclusion of O(alpha_s) supersymmetric QCD (SQCD) corrections within the MSSM. We include the decay of the electroweak gauge boson into dileptons, i.e. we consider the production of charged lepton--anti-lepton or lepton-neutrino final states with one hard jet. We find that the SQCD corrections are negligible for the integrated cross section. Only at high lepton transverse momentum can they induce effects of the percent level.Comment: 21 pages, 9 figures, 2 table

Transport parameters of 2D systems derived from microwave transmission experiments

This paper reports on low temperature microwave transmission experiments which are performed in high magnetic fields on two-dimensional electron gas (2DEG) systems of heterostructure quantum wells. The main transport parameters of the 2DEG, namely, the electron concentration n(s) the mobility my, and the effective mass m*, are evaluated from the transmitted microwave power. We use two alternative configurations to couple the microwaves into the 2DEG: first the sample fills a rectangular waveguide where the microwaves (26.5-40 GHz) propagate parallel to the magnetic field B (Faraday configuration), second, the microwaves (2-18 GHz) are guided by a coplanar structure mounted on the top of the sample which leads to a Voigt configuration. For both arrangements the microwave power transmitted greatly depends on B according to the respective correlation between microwave transmission and the high frequency conductivity tensor sigma of the 2DEG. Well-pronounced Shubnikov-de Haas oscillations are observed. We compare the discussed methods with respect to experimental feasibility, reproducibility, and data extraction

Comparison of different conductive fillers in silicone for the purpose of replacing metallic conductive structures in flexible implants

Graphite (G), Carbon Black (CB) and Carbon Nanotubes (CNT) are compared regarding their usability as conductive filling particles in medical silicone. Produced test structures were characterized mechanically and electrically. CNT turn out to produce the lowest electrical resistance at the lowest concentration. This and the small elongation dependency of the test structure resistance at lengthening up to 6 % cause CNT to be the ideal filler. Therefore CNT filled silicone is the best choice to replace metallic conductive structures in flexible implants