942 research outputs found

    Muon g-2 Anomaly confronted with the higgs global data in the Left-Right Twin Higgs Models

    Full text link
    We will examine the Left-Right Twin Higgs(LRTH) Models as a solution of muon g-2 anomaly with the background of the Higgs global fit data. In the calculation, the joint constrains from the theory, the precision electroweak data, the 125 GeV Higgs data, the leptonic flavor changing decay \mu \to e\gamma decays, and the constraints m_{\nu_R}>m_T>m_{W_H} are all considered. And with the small mass of the \phi^0, the direct searches from the h→ϕ0ϕ0h\to \phi^0\phi^0 channels can impose stringent upper limits on Br(h\to \phi^0\phi^0) and can reduce the allowed region of m_{\phi^0} and f. It is concluded that the muon g-2 anomaly can be explained in the region of 200 GeV \leq M\leq 500 GeV, 700 GeV \leq f\leq 1100 GeV, 13 GeV \leq m_{\phi^0}\leq 55 GeV, 100 GeV \leq m_{\phi^\pm}\leq 900 GeV, and m_{\nu_R}\geq 15 TeV after imposing all the constraints mentioned above.Comment: 18 pages, 4 figures, some typos modifie

    Light axigluon and single top production at the LHC

    Full text link
    The light axigluon model can explain the Tevatron tt‾t\overline{t} forward-backward asymmetry and at the same time satisfy the constraints from the electroweak precision measurement and the ATLASATLAS and CMSCMS data, which induces the flavor changing (FCFC) couplings of axigluon with the SMSM and new quarks. We investigate the effects of these FCFC couplings on the s- and t-channel single top productions at the LHCLHC and the FCFC decays Z→b‾s+bs‾Z\rightarrow \overline{b}s+b\overline{s}, t→cγt\rightarrow c\gamma and cgcg. Our numerical results show that the light axigluon can give significantly contributions to single top production and the rare top decays t→cγt\rightarrow c\gamma and cgcg.Comment: 22 pages, 8 figures; references added, contributions of new quarks to rare decay processes adde

    Associated production of the heavy charged gauge boson WH{W_{H}} and a top quark at LHC

    Full text link
    In the context of topflavor seesaw model, we study the production of the heavy charged gauge boson WH{W_{H}} associated with a top quark at the LHC. Focusing on the searching channel pp→tWH→ttˉb→lνjjbbbpp\rightarrow tW_H\rightarrow t\bar{t}b \rightarrow l\nu jjbbb, we carry out a full simulation of the signal and the relevant standard model backgrounds. The kinematical distributions of final states are presented. It is found that the backgrounds can be significantly suppressed by sets of kinematic cuts, and the signal of the heavy charged boson might be detected at the LHC with s=14\sqrt{s}=14 TeV. With a integrated luminosity of \LL= 100 fb−1fb^{-1}, a 8.3σ8.3 \sigma signal significance can be achieved for mWH=1.6m_{W_H}=1.6 TeV.Comment: 16 pages, 6 figure

    Bottom partner B' and Zb production at the LHC

    Get PDF
    Some new physics models, such as "beautiful mirrors" scenario, predict the existence of the bottom partner B′B'. Considering the constraints from the data for the Z→bbˉZ\rightarrow b\bar{b} branching ratio RbR_{b} and the FBFB asymmetry AFBbA_{FB}^{b} on the relevant free parameters, we calculate the contributions of B′B' to the cross section σ(Zb)\sigma(Zb) and the ZZ polarization asymmetry AZA_{Z} for ZbZb production at the LHCLHC. We find that the bottom partner B′B' can generate significant corrections to σ(Zb)\sigma(Zb) and AZA_{Z}, which might be detected in near future.Comment: 15 pages, 5 figures. Version published in Phys. Lett.

    2-(Dibutyl­amino)-3-(4-fluoro­phen­yl)-5,6,7,8-tetra­hydro-7-methyl-6,8-di­phenyl­pyridine­[3′,4′:2,3]thieno[5,4-d]pyrimidin-4(3H)-one

    Get PDF
    In the crystal structure of the title compound, C36H39FN4OS, the two fused rings of the thienopyrimidine system are coplanar. The 4-fluoro­phenyl ring is twisted with respect to the heterocyclic pyrimidinone ring by 67.21 (14)°. The piperidine ring shows a half-chair conformation. One of the n-butyl chains is disordered equally over two sites. The crystal packing is stabilized by C—H⋯O hydrogen bonds

    Ab initio study of the giant ferroelectric distortion and pressure induced spin-state transition in BiCoO3

    Full text link
    Using configuration-state-constrained electronic structure calculations based on the generalized gradient approximation plus Hubbard U method, we sought the origin of the giant tetragonal ferroelectric distortion in the ambient phase of the potentially multiferroic material BiCoO3 and identified the nature of the pressure induced spin-state transition. Our results show that a strong Bi-O covalency drives the giant ferroelectric distortion, which is further stabilized by an xy-type orbital ordering of the high-spin (HS) Co3+ ions. For the orthorhombic phase under 5.8 GPa, we find that a mixed HS and low-spin (LS) state is more stable than both LS and intermediate-spin (IS) states, and that the former well accounts for the available experimental results. Thus, we identify that the pressure induced spin-state transition is via a mixed HS+LS state, and we predict that the HS-to-LS transition would be complete upon a large volume decrease of about 20%.Comment: 6 pages, 6 figures, 2 table

    Accretion Disk for regular black holes with sub-Planckian curvature

    Full text link
    We investigate the accretion disk for a sort of regular black holes which are characterized by sub-Planckian curvature and Minkowskian core. We derive null geodesics outside the horizon of such regular black holes and analyze the feature of the light rays from the accretion disk which can be classified into direct emission, lensed rings, and photon rings. We find that the observed brightness under different emission models is mainly determined by direct emission, while the contribution from the flux of the lensed and photon rings is limited. By comparing with Bardeen black hole with a dS core, it is found that the black hole with a Minkowskian core exhibits distinct astronomical optical features when surrounded by accretion disk, which potentially provides a way to distinguish these two sorts of black holes by astronomical observation.Comment: 26 pages,9 figure
    • …
    corecore