Study of scalar meson a0(980)a_0(980) from B→a0(980)πB \to a_0(980)π Decays

preprint2009arXivOpen access

Abstract

In this paper, we calculate the branching ratios and the direct CP-violating asymmetries for decays Bˉ0→a00(980)π0,a0+(980)π−,a0−(980)π+\bar{B}^0\to a^0_0(980)π^0, a^+_0(980)π^-, a^-_0(980)π^+ and B−→a00(980)π−,a0−(980)π0B^-\to a^0_0(980)π^-, a^-_0(980)π^0 by employing the perturbative QCD factorization approach. Although the light scalar meson a0(980)a_0(980) is widely perceived as primarily the four-quark bound states, the calculation shows that the 2-quark model supposition for a0(980)a_0(980) can not be ruled out by the currently available experiment upper limits. In these considered decays, the branching ratio for the B−→a00(980)π−B^-\to a^0_0(980)π^- is the largest, 2.8×10−62.8\times 10^{-6}, while its direct CP asymmetry is the smallest, ∼14\sim 14%. Although the direct CP asymmetries for the decays Bˉ0→a00(980)π0,B−→a0−(980)π0\bar{B}^0\to a^0_0(980)π^0, B^-\to a^-_0(980)π^0 are large, about (70∼80)(70\thicksim80)%, it is still difficult to measure them, since their branching ratios are small, around (4∼5)×10−7(4\thicksim5)\times 10^{-7}.

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