19 research outputs found

    Optimal renormalization and the extraction of strange quark mass from semi-leptonic τ\tau-decay

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    We employ optimal renormalization group analysis to semi-leptonic τ\tau-decay polarization functions and extract the strange quark mass from their moments measured by the ALEPH and OPAL collaborations. The optimal renormalization group makes use of the renormalization group equation of a given perturbation series which then leads to closed form sum of all the renormalization group-accessible logarithms which have reduced scale dependence. Using the latest theoretical inputs we find ms(2GeV)=106.70±9.36 MeVm_s(2{\rm GeV}) = 106.70 \pm 9.36~{\rm MeV} and ms(2GeV)=74.47±7.77 MeVm_s(2{\rm GeV}) = 74.47 \pm 7.77~{\rm MeV} for ALEPH and OPAL data respectively.Comment: 3 pages, Contribution to the proceedings of the XXII DAE-BRNS High Energy Physics Symposium, University of Delhi, Dec. 12-16, 201

    Beautiful Mirrors at the LHC

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    We explore the "Beautiful Mirrors" model, which aims to explain the measured value of AFBbA^b_{FB}, discrepant at the 2.9σ2.9\sigma level. This scenario introduces vector-like quarks which mix with the bottom, subtly affecting its coupling to the ZZ. The spectrum of the new particles consists of two bottom-like quarks and a charge -4/3 quark, all of which have electroweak interactions with the third generation. We explore the phenomenology and discovery reach for these new particles at the LHC, exploring single mirror quark production modes whose rates are proportional to the same mixing parameters which resolve the AFBbA_{FB}^b anomaly. We find that for mirror quark masses 500GeV,a14TeVLHCwith300fb1\lesssim 500 GeV, a 14 TeV LHC with 300 {\rm fb}^{-1} is required to reasonably establish the scenario and extract the relevant mixing parameters.Comment: version to be published in JHE

    Anomalous tqγtq\gamma coupling effects in exclusive radiative B-meson decays

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    The top-quark FCNC processes will be searched for at the CERN LHC, which are correlated with the B-meson decays. In this paper, we study the effects of top-quark anomalous interactions tqγtq\gamma in the exclusive radiative BKγB\to K^*\gamma and BργB\to\rho\gamma decays. With the current experimental data of the branching ratios, the direct CP and the isospin asymmetries, bounds on the coupling κtcRγ\kappa_{tcR}^{\gamma} from BKγB\to K^*\gamma and κtuRγ\kappa_{tuR}^{\gamma} from BργB\to \rho\gamma decays are derived, respectively. The bound on κtcRγ|\kappa_{tcR}^{\gamma}| from B(BKγ){\mathcal B}(B\to K^{*}\gamma) is generally compatible with that from B(BXsγ){\mathcal B}(B\to X_{s}\gamma). However, the isospin asymmetry Δ(Kγ)\Delta(K^{*}\gamma) further restrict the phase of κtcRγ\kappa_{tcR}^{\gamma}, and the combined bound results in the upper limit, B(tcγ)<0.21\mathcal B(t\to c\gamma)<0.21%, which is lower than the CDF result. For real κtcRγ\kappa_{tcR}^{\gamma}, the upper bound on B(tcγ)\mathcal B(t\to c\gamma) is about of the same order as the 5σ5\sigma discovery potential of ATLAS with an integrated luminosity of 10fb110 {\rm fb}^{-1}. For BργB\to\rho\gamma decays, the NP contribution is enhanced by a large CKM factor Vud/Vtd|V_{ud}/V_{td}|, and the constraint on tuγtu\gamma coupling is rather restrictive, B(tuγ)<1.44×105\mathcal B(t\to u\gamma)<1.44\times 10^{-5}. With refined measurements to be available at the LHCb and the future super-B factories, we can get close correlations between BVγB\to V \gamma and the rare tqγt\to q\gamma decays, which will be studied directly at the LHC ATLAS and CMS.Comment: 25 pages, 15 figures, pdflate

    The possible functions of duplicated ets (GGAA) motifs located near transcription start sites of various human genes

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    Transcription is one of the most fundamental nuclear functions and is an enzyme complex-mediated reaction that converts DNA sequences into mRNA. Analyzing DNA sequences of 5′-flanking regions of several human genes that respond to 12-O-tetradecanoyl-phorbol-13-acetate (TPA) in HL-60 cells, we have identified that the ets (GGAA) motifs are duplicated, overlapped, or clustered within a 500-bp distance from the most 5′-upstream region of the cDNA. Multiple protein factors including Ets family proteins are known to recognize and bind to the GGAA containing sequences. In addition, it has been reported that the ets motifs play important roles in regulation of various promoters. Here, we propose a molecular mechanism, defined by the presence of duplication and multiplication of the GGAA motifs, that is responsible for the initiation of transcription of several genes and for the recruitment of binding proteins to the transcription start site (TSS) of TATA-less promoters

    Search for the Λb0Λη\Lambda^0_b \rightarrow \Lambda \eta^\prime and Λb0Λη\Lambda^0_b \rightarrow \Lambda \eta decays with the LHCb detector

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    A search is performed for the as yet unobserved baryonic ΛbΛη\Lambda_b \rightarrow \Lambda \eta^\prime and ΛbΛη\Lambda_b \rightarrow \Lambda \eta decays with 3fb1fb^{-1} of proton-proton collision data recorded by the LHCb experiment. The B0KS0ηB^0 \rightarrow K_S^0 \eta^\prime decay is used as a normalisation channel. No significant signal is observed for the ΛbΛη\Lambda_b \rightarrow \Lambda \eta^\prime decay. An upper limit is found on the branching fraction of B(ΛbΛη)<3.1×106\mathcal{B}(\Lambda_b \rightarrow \Lambda \eta^\prime)<3.1\times10^{-6}} at 90\% confidence level. Evidence is seen for the presence of the ΛbΛη\Lambda_b \rightarrow \Lambda \eta decay at the level of 3σ3\sigma significance, with a branching fraction B(ΛbΛη)=(9.35.3+7.3)×106\mathcal{B}(\Lambda_b \rightarrow \Lambda \eta)=(9.3^{+7.3}_{-5.3})\times10^{-6}}.Comment: 22 pages, 6 figures. v2 is published version (very minor revisions
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