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Branching Ratio and CP Asymmetry of B_s \to K^*_0(1430)\pi Decays in the PQCD Approach

Abstract

In the two-quark model supposition for K0βˆ—(1430)K_0^{*}(1430), the branching ratios and the direct CP-violating asymmetries for decays BΛ‰s0β†’K0βˆ—0(1430)Ο€0,K0βˆ—+(1430)Ο€βˆ’\bar B_s^0\to K^{*0}_0(1430)\pi^0, K^{*+}_0(1430)\pi^- are studied by employing the perturbative QCD factorization approach. We find that although these two decays are both tree-dominated, the ratio of their penguin to tree contributions are very different: there is only a few percent for the decay BΛ‰s0β†’K0βˆ—+(1430)Ο€βˆ’\bar B_s^0\to K^{*+}_0(1430)\pi^-, while about 37% in scenario I, even 51% in scenario II for the decay BΛ‰s0β†’K0βˆ—0(1430)Ο€0\bar B_s^0\to K^{*0}_0(1430)\pi^0. It results that these two decays have very different values in the branching ratios and the direct CP asymmetries. The branching ratio of the decay BΛ‰s0β†’K0βˆ—+(1430)Ο€βˆ’\bar B_s^0\to K^{*+}_0(1430)\pi^- is at the order of 10βˆ’510^{-5}, and its direct CP asymmetry is about (20-30)%. While for the decay BΛ‰s0β†’K0βˆ—0(1430)Ο€0\bar B_s^0\to K^{*0}_0(1430)\pi^0, its direct CP-violating asymmetry is very large and about 90%, but it is difficult to measure it, because the branching ratio for this channel is small and only 10βˆ’710^{-7} order.Comment: 8pages, 2figure

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