144,372 research outputs found

    The Electromagnetic Decays of BcΒ±(2S)B^{\pm}_c(2S)

    Full text link
    We calculate the electromagnetic (EM) decay widths of the BcΒ±(2S)B^{\pm}_c(2S) meson, which is observed recently by the ATLAS Collaboration. The main EM decay channels of this particle are 13S1Ξ³1{^3S_1}\gamma and 1PΞ³1{P}\gamma, which, in literature, are estimated to have the branching ratio of about 1/101/10. In this work, we get the partial decay widths: Ξ“(21S0β†’13S1Ξ³)=0.192\Gamma(2{^1S_0}\rightarrow 1{^3S_1}\gamma)=0.192 keV, Ξ“(21S0β†’1P1Ξ³)=2.24\Gamma(2{^1S_0}\rightarrow 1{P_1}\gamma) = 2.24 keV and Ξ“(21S0β†’1P1β€²Ξ³)=11.4\Gamma(2{^1S_0}\rightarrow 1{P_1^\prime}\gamma) = 11.4 keV. In the calculation, the instantaneous approximated Bethe-Salpeter method is used. For the PP-wave BcB_c mesons, the wave functions are given by mixing the 3P1^3P_1 and 1P1^1P_1 states. Within the Mandelstam formalism, the decay amplitude is given, which includes the relativistic corrections.Comment: 9 pages, 3 figures, 3 table

    The study of light invisible particles in BcB_c decays

    Full text link
    In this paper, we study the light scalar and pseudoscalar invisible particles in the flavor changing neutral current processes of the BcB_c meson. Effective operators are introduced to describe the couplings between quarks and light invisible particles. The Wilson coefficients are extracted from the experimental results of the BB and DD mesons, which are used to predict the upper limits of the branching fractions of the similar decay processes for the BcB_c meson. The hadronic transition matrix element is calculated with the instantaneously approximated Bethe-Salpeter method. The upper limits of the branching fractions when mΟ‡m_\chi taking different values are presented. It is found that at some region of mΟ‡m_\chi, the channel Bcβ†’Ds(βˆ—)χχB_c\to D_s^{(\ast)}\chi\chi has the largest upper limit which is of the order of 10βˆ’610^{-6}, and for Bcβ†’Dsβˆ—Ο‡Ο‡β€ B_c\to D_s^\ast\chi\chi^\dagger, the largest value of the upper limits can achieve the order of 10βˆ’510^{-5}. Other decay modes, such as Bcβ†’D(βˆ—)χχ(†)B_c\to D^{(*)}\chi\chi^{(\dagger)} and Bcβ†’B(βˆ—)χχ(†)B_c\to B^{(*)}\chi\chi^{(\dagger)}, are also considered.Comment: 24 pages, 35 figure
    • …
    corecore