7,370 research outputs found

    Top Quark Measurements at the Fermilab Tevatron

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    The top quark, discovered at the Tevatron in 1995, is a very interesting particle. Precise measurement of the top properties using large data samples will allow stringent tests of the Standard Model and offer a unique window on new physics. In this report will be reviewed the status of the current knowledge of the top quark as provided by the Run I results of the CDF and D0 experiment. A first look at various preliminary measurements obtained with data collected during Run II will be also presented.Comment: 10 pages, 14 figures Proceeding of Lepton-Photon 2003, Fermilab Batavia (IL), August 200

    First look at the physics case of TLEP

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    The discovery by the ATLAS and CMS experiments of a new boson with mass around 125 GeV and with measured properties compatible with those of a Standard-Model Higgs boson, coupled with the absence of discoveries of phenomena beyond the Standard Model at the TeV scale, has triggered interest in ideas for future Higgs factories. A new circular e+e− collider hosted in a 80 to 100km tunnel, TLEP, is among the most attractive solutions proposed so far. It has a clean experimental environment, produces high luminosity for top-quark, Higgs boson, Wand Z studies, accommodates multiple detectors, and can reach energies up to the t¯t threshold and beyond. It will enable measurements of the Higgs boson properties and of Electroweak Symmetry-Breaking (EWSB) parameters with unequalled precision, offering exploration of physics beyond the Standard Model in the multi-TeV range. Moreover, being the natural precursor of the VHE-LHC, a 100TeV hadron machine in the same tunnel, it builds up a long-term vision for particle physics

    Comments on "Wall-plug (AC) power consumption of a very high energy e+/e- storage ring collider" by Marc Ross

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    The paper arXiv:1308.0735 questions some of the technical assumptions made by the TLEP Steering Group when estimating in arXiv:1305.6498 the power requirement for the very high energy e+e- storage ring collider TLEP. We show that our assumptions are based solidly on CERN experience with LEP and the LHC, as well accelerators elsewhere, and confirm our earlier baseline estimate of the TLEP power consumption.Comment: 6 page

    Fluorochrome Interaction with the Mitochondrial Membrane THE EFFECT OF ENERGY CONSERVATION

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    Abstract The interaction of 1-anilino-8-naphthalenesulfonate and 6-p-toluidino-2-naphthalenesulfonate with the membrane of both mitochondria and submitochondrial particles was studied. A fluorescence increase of the added fluorochromes was observed when energy was supplied to the membrane of submitochondrial particles, while a fluorescence decrease was observed with intact mitochondria. Binding studies and a comparison of the two fluorochromes have indicated that polarity changes of the membrane are not measured by 1-anilino-8-naphthalenesulfonate and 6-p-toluidino-2-naphthalenesulfonate. The fluorescence changes associated with energy conservation can be attributed to changes in the binding of the fluorochromes. Either a conformational change or a membrane potential change could account for the results

    Physics Behind Precision

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    This document provides a writeup of contributions to the FCC-ee mini-workshop on "Physics behind precision" held at CERN, on 2-3 February 2016.Comment: https://indico.cern.ch/event/469561

    Unifying gauge couplings at the string scale

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    Using the current precision electroweak data, we look for the minimal particle content which is necessary to add to the standard model in order to have a complete unification of gauge couplings and gravity at the weakly coupled heterotic string scale. We find that the addition of a vector-like fermion at an intermediate scale and a non-standard hypercharge normalization are in general sufficient to achieve this goal at two-loop level. Requiring the extra matter scale to be below the TeV scale, it is found that the addition of three vector-like fermion doublets with a mass around 700 GeV yields a perfect string-scale unification, provided that the affine levels are (kY,k2,k3)=(13/3,1,2)(k_Y, k_2 ,k_3)=(13/3, 1, 2) , as in the SU(5)×SU(5)SU(5) \times SU(5) string-GUT. Furthermore, if supersymmetry is broken at the unification scale, the Higgs mass is predicted in the range 125 GeV - 170 GeV, depending on the precise values of the top quark mass and tan⁥ÎČ\tan \beta parameter.Comment: 11 pages, 4 eps figures, using jpconf style, talk given at CORFU2005, RTN meeting ``The Quest for Unification: Theory Confronts Experiment'', 11 - 18 September 2005, Corfu, Greec
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