4,366 research outputs found

    Bsϕl+lB_s \to \phi l^+ l^- decays in the topcolor-assisted technicolor model

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    Using the updated form factors within the light-cone QCD sum rule approach, we calculate the new physics contributions to rare semileptonic Bˉsϕμ+μ,ϕτ+τ\bar{B}_s \to \phi\mu^+\mu^-, \phi \tau^+\tau^- decays from the new particles appearing in the topcolor-assisted technicolor (TC2) model. In our evaluations, we find that: (i) the branching ratio, normalized forward-backward asymmetry and lepton polarization show highly sensitivity to charged top-pions contributions and little sensitivity to ZZ' contributions. The TC2 enhancements to the branching ratios of these decays can reach a factor of 242 \sim 4; (ii) the NP enhancement to the forward-backward asymmetry of the decay Bsϕμ+μB_s\to \phi \mu^+\mu^- is in the range -9% to 22%, but -10% to 0% for decay Bsϕτ+τB_s\to \phi \tau^+\tau^- compared to the SM predictions; (iii) the TC2 model provide an enhancement of more than 30% to the longitudinal polarization asymmetry PLP_L for decay Bsϕμ+μB_s\to \phi \mu^+\mu^-, but a decrease of about 20% to the transverse polarization asymmetry PTP_T for the decay Bsϕτ+τB_s\to \phi \tau^+\tau^-.Comment: 19 pages, 6 figures, figures changed, two references adde

    Ultra-low noise magnetic field for quantum gases

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    Ultra-low noise magnetic field is essential for many branches of scientific research. Examplesinclude experiments conducted on ultra-cold atoms, quantum simulations, as well as precisionmeasurements. In ultra-cold atom experiments specifically, a bias magnetic field will be oftenserved as a quantization axis and be applied for Zeeman splitting. As atomic states areusually sensitive to magnetic fields, a magnetic field characterized by ultra-low noise as wellas high stability is typically required for experimentation. For this study, a bias magneticfield is successfully stabilized at 14.5G, with the root mean square (RMS) value of the noisereduced to 18.5{\mu}G (1.28ppm) by placing{\mu}-metal magnetic shields together with a dynamicalfeedback circuit. Long-time instability is also regulated consistently below 7{\mu}G. The level ofnoise exhibited in the bias magnetic field is further confirmed by evaluating the coherencetime of a Bose-Einstein condensate characterized by Rabi oscillation. It is concluded thatthis approach can be applied to other physical systems as well.Comment: 7 pages, 5 figure

    Semileptonic Decays of BcB_c Meson to a P-Wave Charmonium State χc\chi_c or hch_c

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    The semileptonic decays of meson BcB_c to a P-wave charmonium state χc(3PJ)\chi_c(^3P_J) or hc(1P1)h_c(^1P_1) are computed. The results show that the decays are sizable so they are accessible in Tevatron and in LHC, especially, with the detectors LHCB and BTeV in the foreseeable future, and of them, the one to the 1P1^1P_1 charmonium state potentially offers us a novel window to see the unconfirmed hch_c particle. In addition, it is pointed out that since the two charmonium radiative decays χc(3P1,2)J/ψ+γ\chi_c(^3P_{1,2}) \to J/\psi+\gamma have sizable branching ratios, the cascade decays of the concerned decays and the charmonium radiative decays may affect the result of the observing the BcB_c meson through the semileptonic decays BcJ/ψ+l+νlB_{c}\to {J/\psi}+{l}+\nu_{l} substantially.Comment: 8 pages, 2 figure

    The Pure Leptonic Decays of B_c Meson and Their Radiative Corrections

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    The radiative corrections to the pure leptonic decay BcνB_c \to \ell\nu_{\ell} up-to one-loop order is presented. How to cancel the infrared divergences appearing in the loop calculations, and the radiative decay BcνγB_c \to \ell\nu_{\ell}\gamma is shown precisely. It is emphasized that the radiative decay may be separated properly and may compare with measurements directly as long as the theoretical `softness' of the photon corresponds to the experimental resolutions. Furthermore with a kind of non-relativistic constituent quark model, a kind of typical long distance contributions to the radiative decays is estimated, and it is shown that the contributions are negligible in comparison with the accuracy of one-loop corrections and the expected experimental measurements.Comment: 20 pages including 6 figures, REVTe
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