Estimating decay rate of X±(5568)→Bsπ±X^{\pm}(5568)\to B_sπ^{\pm} while assuming them to be molecular states

preprint2018arXivOpen access

Abstract

Discovery of X(5568)X(5568) brings up a tremendous interest because it is very special, i.e. made of four different flavors. The D0 collaboration claimed that they observed this resonance through portal X(5568)→BsπX(5568)\to B_sπ, but unfortunately, later the LHCb, CMS, CDF and ATLAS collaborations' reports indicate that no such state was found. Almost on the Eve of 2017, the D0 collaboration reconfirmed existence of X(5568)X(5568) via the semileptonic decay of BsB_s. To further reveal the discrepancy, supposing X(5568)X(5568) as a molecular state, we calculate the decay rate of X(5568)→Bsπ+X(5568)\rightarrow B_sπ^+ in an extended light front model. Numerically, the theoretically predicted decay width of Γ(X(5568)→Bsπ+)Γ(X(5568)\rightarrow B_sπ^+) is 20.2820.28 MeV which is consistent with the result of the D0 collaboration (Γ=18.6−6.1+7.9(stat)−3.8+3.5(syst)Γ=18.6^{+7.9}_{-6.1}(stat)^{+3.5}_{-3.8}(syst) MeV). Since the resonance is narrow, signals might be drowned in a messy background. In analog, two open-charm molecular states DKDK and BDBD named as XaX_a and XbX_b, could be in the same situation. The rates of Xa→Dsπ0X_a\to D_sπ^0 and Xb→Bcπ0X_b\to B_cπ^0 are estimated as about 30 MeV and 20 MeV respectively. We suggest the experimental collaborations round the world to search for these two modes and accurate measurements may provide us with valuable information.

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