868 research outputs found

    Light spin-1/2 or spin-0 Dark Matter particles

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    We recall and precise how light spin-0 particles could be acceptable Dark Matter candidates, and extend this analysis to spin-1/2 particles. We evaluate the (rather large) annihilation cross sections required, and show how they may be induced by a new light neutral spin-1 boson U. If this one is vectorially coupled to matter particles, the (spin-1/2 or spin-0) Dark Matter annihilation cross section into e+e- automatically includes a v_dm^2 suppression factor at threshold, as desirable to avoid an excessive production of gamma rays from residual Dark Matter annihilations. We also relate Dark Matter annihilations with production cross sections in e+e- scatterings. Annihilation cross sections of spin-1/2 and spin-0 Dark Matter particles are given by exactly the same expressions. Just as for spin-0, light spin-1/2 Dark Matter particles annihilating into e+e- could be responsible for the bright 511 keV gamma ray line observed by INTEGRAL from the galactic bulge.Comment: 10 page

    Upstream stimulators for recoding

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    Journal ArticleRecent progress in elucidation of 5' stimulatory elements for translational recoding is reviewed. A 5' Shine-Dalgarno sequence increases both +l and ? I frameshift efficiency in several genes; examples cited include the E. coli prfB gene encoding release factor 2 and the thuiX gene encoding the y and t subunits of DNA polymerase III holoenzyme. The spacing between the Shine-Dalgarno sequence and the shift site is critical in both the +l and ? 1 frameshift cassettes; however, the optimal spacing is quite different in the two cases. A frameshift in a mammalian chromosomal gene, ornithine decarboxylase antizyme, has recently been reported; 5' sequences have been shown to be vital for this frameshift event. Escherichia coli bacteriophage T4 gene 60 encodes a subunit of its type II DNA topoisomerase. The mature gene 60 mRNA contains an internal 50 nucleotide region that appears to be bypassed during translation. A 16 amino acid domain of the nascent peptide is necessary for this bypass to occur

    Non-Minimal and Non-Universal Supersymmetry

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    I motivate and discuss non-minimal and non-universal models of supersymmetry and supergravity consistent with string unification at 101610^{16} GeV.Comment: 10 pages, Latex. Plenary talk given at 6th Workshop in High Energy Physics Phenomenology (WHEPP 6), Chennai (Madras), India, 3-15 Jan 200

    Study of the Gauge Mediation Signal with Non-pointing Photons at the CERN LHC

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    In this paper we study the gauge mediation signal with the ATLAS detector at the CERN LHC. We focus on the case where the NLSP is the long-lived lightest neutralino (χ~10\tilde{\chi}^0_1) which decays dominantly into a photon (Îł\gamma) and a gravitino (G~\tilde{G}). A non-pointing photon from the neutralino decay can be detected with good position and time resolutions by the electormagnetic calorimeter (ECAL), while the photon momentum would be precisely measured if the photon is converted inside the inner tracking detector before reaching the ECAL. A new technique is developed to determine the masses of the slepton (ℓ~\tilde{\ell}) and the neutralino from events with a lepton and a converted non-pointing photon arising from the cascade decay ℓ~→ℓχ~10→ℓγG~\tilde{\ell}\to \ell\tilde{\chi}^0_1\to \ell\gamma \tilde{G}. A Monte Carlo simulation at a sample point shows that the masses would be measured with an error of 3% for O\cal{O}(100) selected ℓγ\ell\gamma pairs. Once the sparticle masses are determined by this method, the decay time and momentum of the neutralino are solved using the ECAL data and the lepton momentum only, for all ℓγ\ell\gamma pairs without the photon conversion. We estimate the sensitivity to the neutralino lifetime for cτ=10c\tau=10 cm to O\cal{O}(10) m.Comment: 19 page, 7 figures, revte

    On non-universal Goldstino couplings to matter

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    Using the constrained superfields formalism to describe the interactions of a light goldstino to matter fields in supersymmetric models, we identify generalised, higher-order holomorphic superfield constraints that project out the superpartners and capture the non-universal couplings of the goldstino to matter fields. These arise from microscopic theories in which heavy superpartners masses are of the order of the supersymmetry breaking scale (\sqrt f). In the decoupling limit of infinite superpartners masses, these constraints reduce to the familiar, lower-order universal constraints discussed recently, that describe the universal goldstino-matter fields couplings, suppressed by inverse powers of \sqrt f. We initiate the study of the couplings of the Standard Model (SM) fields to goldstino in the constrained superfields formalism.Comment: 28 pages; one comment adde

    LHC Reach for Gauge Mediated Supersymmetry Breaking Models Via Prompt Photon Channels

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    We evaluate the supersymmetry reach of the Large Hadron Collider within the gauge-mediated low energy supersymmetry breaking framework, assuming that a neutralino is the second lightest sparticle and that it decays promptly into a gravitino which escapes detection. We find that the maximum reach is obtained via a search for inclusive \gamma\gamma+\eslt events coming dominantly from chargino and neutralino production. Assuming an integrated luminosity of 10~fb−1fb^{-1}, we find that LHC experiments will be able to probe values of the model parameter \Lambda \alt 400 TeV, corresponding to mtg⁥≀2.8m_{\tg} \leq 2.8 TeV. A measure of the model parameter Λ\Lambda may be possible from the photon pTp_T spectrum.Comment: 10 page Revtex file plus 4 EPS figure

    Fitting Neutrino Physics with a U(1)_R Lepton Number

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    We study neutrino physics in the context of a supersymmetric model where a continuous R-symmetry is identified with the total Lepton Number and one sneutrino can thus play the role of the down type Higgs. We show that R-breaking effects communicated to the visible sector by Anomaly Mediation can reproduce neutrino masses and mixing solely via radiative contributions, without requiring any additional degree of freedom. In particular, a relatively large reactor angle (as recently observed by the Daya Bay collaboration) can be accommodated in ample regions of the parameter space. On the contrary, if the R-breaking is communicated to the visible sector by gravitational effects at the Planck scale, additional particles are necessary to accommodate neutrino data.Comment: 19 pages, 3 figures; v2: references added, constraints updated, overall conclusions unchange
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