paper

Revisiting charmless hadronic B decays to scalar mesons

arXiv:1303.4403 · doi:10.1103/PhysRevD.87.114001

Abstract

Hadronic charmless B decays to scalar mesons are studied within the framework of QCD factorization (QCDF). Considering two different scenarios for scalar mesons above 1 GeV, we find that the data favor the scenario in which the scalars and are the lowest lying bound states. This in turn implies a preferred four-quark nature for light scalars below 1 GeV. Assuming being a lowest lying state, we show that the data of and can be accommodated in QCDF without introducing power corrections induced from penguin annihilation, while the predicted $B^-\to \ov K_0^{*0}(1430)π^-$ and $\ov B^0\to K_0^{*-}(1430)π^+$ are too small compared to experiment. In principle, the data of modes can be explained if penguin-annihilation induced power corrections are taken into account. However, this will destroy the agreement between theory and experiment for . Contrary to the pseudoscalar meson sector where has the largest rate in 2-body decays of the meson, we show that $Br(B\to K_0^*η')<\B(B\to K_0^*η)$. The decay $\ov B^0\to a_0(980)^+K^-$ is found to have a rate much smaller than that of $\ov B^0\to a_0(980)^+π^-$ in QCDF, while it is the other way around in pQCD. Experimental measurements of these two modes will help discriminate between these two different approaches. Assuming 2-quark bound states for and , the observed large rates of and modes can be explained in QCDF with the mixing angle in the vicinity of .

25 pages, 3 figures

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