1,434 research outputs found

    kTk_T-factorization approach to the Higgs boson production in ZZβˆ—β†’4β„“ZZ^*\to 4\ell channel at the LHC

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    We calculated a differential cross section of the Higgs boson production in the hβ†’ZZβˆ—β†’4β„“h\to ZZ^*\to 4\ell decay channel within the framework of kTk_T-factorization. Results are obtained using an off-shell matrix element for the gβˆ—gβˆ—β†’hβ†’ZZβˆ—β†’4β„“g^*g^*\to h\to ZZ^*\to 4\ell process together with Ciafaloni-Catani-Fiorani-Marchesini (CCFM) evolution equations for an unintegrated gluon distribution function. We have presented a comparison of our results with the latest experimental measurements at S\sqrt{S} = 8 TeV and S\sqrt{S} = 13 TeV from the ATLAS and CMS collaborations at the LHC. In addition to this, we have compared our results with the results from the collinear factorization formalism calculated up to next-to-next-to-leading order plus next-to-next-to-leading logarithm (NNLO + NNLL) accuracy obtained using the HRes code for the Higgs boson production in the gluon-gluon fusion process. Our estimates are consistently close to NNLO + NNLL results obtained using a collinear factorization formalism and are also in agreement with experimental measurements.Comment: 10 pages, 5 figures updated using TMDli

    Minimal Spin-3/2 Dark Matter in a simple ss-channel model

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    We consider a spin~-~3/2 fermionic dark matter candidate (DM) interacting with Standard Model fermions through a vector mediator in the ss-channel. We find that for pure vector couplings almost the entire parameter space of the DM and mediator mass consistent with the observed relic density is ruled out by the direct detection observations through DM-nucleon elastic scattering cross-sections. In contrast, for pure axial-vector coupling, the most stringent constraints are obtained from mono-jet searches at the Large Hadron Collider.Comment: 8 pages, 5 figures, Version accepted for publication in EPJ

    Spin-3/2 dark matter in a simple tt-channel model

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    We consider a spin-3/2 fermionic dark matter (DM) particle interacting with the Standard Model quarks through the exchange of a charged and coloured scalar or vector mediator in a simple tt-channel model. It is found that for the vector mediator case, almost the entire parameter space allowed by the observed relic density is already ruled out by the direct detection LUX data. No such bounds exist on the interaction mediated by scalar particles. Monojet + missing energy searches at the Large Hadron Collider provide the most stringent bounds on the parameters of the model for this case. The collider bounds put a lower limit on the allowed DM masses.Comment: Published EPJC versio

    Probing anomalous couplings using di-Higgs production in electron-proton collisions

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    A proposed high energy Future Circular Hadron-Electron Collider would provide sufficient energy in a clean environment to probe di-Higgs production. Using this channel we show that the azimuthal angle correlation between the missing transverse energy and the forward jet is a very good probe for the non-standard hhhhhh and hhWWhhWW couplings. We give the exclusion limits on these couplings as a function of integrated luminosity at a 9595\% C.L. using the fiducial cross sections. With appropriate error fitting methodology we find that the Higgs boson self coupling could be measured to be ghhh(1)=1.00βˆ’0.17(0.12)+0.24(0.14)g^{(1)}_{hhh} = 1.00^{+0.24(0.14)}_{-0.17(0.12)} of its expected Standard Model value at s=3.5(5.0)\sqrt s = 3.5(5.0) TeV for an ultimate 10 abβˆ’1^{-1} of integrated luminosity

    Identification of rRNA processing gene homologs of yeast in Neurospora crassa

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    Identification of rRNA processing gene homologs of yeast in Neurospora crass
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