49 research outputs found

    Phenomenology of flavorful composite vector bosons in light of BB anomalies

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    We analyze the flavor structure of composite vector bosons arising in a model of vectorlike technicolor, often called hypercolor (HC), with eight flavors that form a one-family content of HC fermions. Dynamics of the composite vector bosons, referred to as HC rho in this paper, are formulated together with HC pions by the hidden local symmetry (HLS), in a way analogous to QCD vector mesons. Then coupling properties to the standard model (SM) fermions, which respect the HLS gauge symmetry, are described in a way that couplings of the HC rhos to the left-handed SM quarks and leptons are given by a well-defined setup as taking the flavor mixing structures into account. Under the present scenario, we discuss significant bounds on the model from electroweak precision tests, flavor physics, and collider physics. We also try to address B anomalies in processes such as B -> K(*) mu+ mu- and B -> D(*) tau nu, recently reported by LHCb, Belle, (ATLAS, and CMS in part.) Then we find that the present model can account for the anomaly in B -> K(*) mu+ mu- consistently with the other constraints while it predicts no significant deviations in B -> D(*) tau nu from the SM, which can be examined in the future Belle II experiment. The former is archived with the form C9 = -C10 of the Wilson coefficients for effective operators of b -> s mu+ mu-, which has been favored by the recent experimental data. We also investigate current and future experimental limits at the Large Hadron Collider (LHC) and see that possible collider signals come from dijet and ditau, or dimuon resonant searches for the present scenario with TeV mass range. To conclude, the present b -> s mu+ mu- anomaly is likely to imply discovery of new vector bosons in the ditau or dimuon channel in the context of the HC rho model. Our model can be considered as a UV completion of conventional U(1)' model.Comment: 62 pages, 8 figures, 3 tables, typos modified, published versio

    Constraint on Universal Extra Dimensions from scalar boson searches

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    We show the bounds on five- and six-dimensional Universal Extra Dimension models from the result of the Higgs boson searches at the Large Hadron Collider and electroweak precision measurement. The latest data released by the ATLAS and the CMS gives the lower bounds on Kaluza-Klein scale which are from 650 GeV to 1350 GeV depending on models from Higgs to diboson/diphoton decay signal. The Higgs production cross section can be enhanced by factor 1.5 in crude estimation, diphoton decay signal is suppressed about 10%. Electroweak precision measurement also gives the lower bounds as from 700 GeV to 1500 GeV.Comment: 4 pages, 1 figure, 1 table, Proceedings of the conference "Rencontres de Moriond EW 2013", La Thuile, Italy, 2-9 Mar. 201

    Tau longitudinal polarization in B -> D tau nu and its role in the search for charged Higgs boson

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    We study the longitudinal polarization of the tau lepton in B -> D tau nu decay. After discussing possible sensitivities of tau decay modes to the tau polarization, we examine the effect of charged Higgs boson on the tau polarization in B -> D tau nu. We find a relation between the decay rate and the tau polarization, and clarify the role of the tau polarization measurement in the search for the charged Higgs boson.Comment: 17 pages, 3 figures. Tau -> l nu nu is included in Sec. II. Accordingly the title is changed. References are adde

    Universal extra dimensions after Higgs discovery

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    We show bounds on five- and six-dimensional universal extra dimension (UED) models from the latest results of the Higgs searches at the LHC and from the electroweak precision data for the S and T parameters. We consider the minimal UED model in five dimensions and the ones in six dimensions. The highest possible ultraviolet cutoff scale for each UED model is evaluated from the electroweak vacuum stability by solving the renormalization group equation of the Higgs self-coupling. This scale turns out to be lower than the conventional one obtained from the perturbativity of the gauge coupling. The resultant 95% C.L. lower bounds on the first Kaluza-Klein scale from the LHC results and from the S, T analysis are 600 and 700 GeV in the minimal UED model, while those in the six-dimensional UED models are 800-1300 GeV and 900-1500 GeV, respectively.Comment: 37 pages, 9 figures, 7 tables (v1); 38 pages, 9 figures, 7 tables, with minor modifications, typos fixed, references added (v2); 37 pages, 10 figures, 7 tables, published version in PRD, figures modified, a figure added, typos fixed, a reference added (v3

    Global fit to b→cτνb \to c\tau\nu anomalies 2022 mid-autumn

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    Recently, the LHCb collaboration announced a preliminary result of the test of lepton flavor universality (LFU) in B→D(∗)B\to D^{(\ast)} semi-leptonic decays: RDLHCb2022=0.441±0.089R_{D}^{\rm LHCb2022} = 0.441 \pm 0.089 and RD∗LHCb2022=0.281±0.030R_{D^{\ast}}^{\rm LHCb2022} = 0.281 \pm 0.030 based on the LHC Run 1 data. This is the first result of RDR_{D} for the LHCb experiment, and its precision is comparable to the other BB-factory data. Interestingly, those data prefer the violation of the LFU again. A new world average of the data from the BaBar, Belle, and LHCb collaborations is RD=0.358±0.027R_{D} = 0.358 \pm 0.027 and RD∗=0.285±0.013R_{D^{\ast}} = 0.285 \pm 0.013. Including this new data, we update a circumstance of the b→cτν‾b \to c \tau \overline\nu measurements and their implications for new physics. Incorporating recent developments for the B→D(∗)B \to D^{(\ast)} form factors in the Standard Model (SM), we observe a 4.1σ4.1 \sigma deviation from the SM predictions. Our updates also include; model-independent new physics (NP) formulae for the related observables; and the global fittings of parameters for leptoquark scenarios as well as single NP operator scenarios. Furthermore, we show future potential to indirectly distinguish different new physics scenarios with the use of the precise measurements of the polarization observables in B→D(∗)τν‾B\to D^{(\ast)}\tau \overline\nu at the Belle II and the high-pTp_{\rm T} flavored-tail searches at the LHC. We also discuss an impact on the LFU violation in Υ→l+l−\Upsilon \to l^+ l^-.Comment: 38 pages, 5 figures, 6 Tables; v2: references adde
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