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首页> 外文期刊>The European Physical Journal, A. Hadrons and Nuclei >Twist-3 light-cone distribution amplitudes of the scalar mesons within the QCD sum rules and their application to the B → S transition form factors
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Twist-3 light-cone distribution amplitudes of the scalar mesons within the QCD sum rules and their application to the B → S transition form factors

机译:QCD和规则内标量介子的Twist-3视锥分布振幅及其在B→S过渡形状因子中的应用

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摘要

We investigate the twist-3 light-cone distribution amplitudes (LCDAs) of the scalar mesons a_0, K_0~? and f_0 within the QCD sum rules. The QCD sum rules are improved by a consistent treatment of the sizable s-quark mass effects within the framework of the background field approach. Adopting the valence quark component (-bar1q2) as the dominant structure of the scalar mesons, our estimation for their masses is close to the measured a_0(1450), K_0~? (1430) and f_0(1710). From the sum rules, we obtain the first two non-zero moments of the twist-3 LCDAs φ_(a_0)~s,σ: 〈ξ_(s,a_0)~(2(4))〉 = 0.369 (0.245) and 〈ξ_(σ,a_0)~(24))〉 = 0.203 (0.093); those of the twist-3 LCDAs φ_(K_0~?)~(s,σ): 〈ξ_(s,K_0~?)~(1(2))〉 = 0.004 (0.355) and 〈ξ_(σ,K_0~?)~(1(2))〉 = 0.018 (0.207); and those of the twist-3 LCDAs φ_(f_0)~(s,σ): 〈ξ_(s,f_0)~(2(4))〉 = 0.335 (0.212) and 〈ξ_(σ,f_0)~(2(4))〉 = 0.196 (0.088), respectively. As an application of those twist-3 LCDAs, we study the B → S transition form factors by introducing proper chiral currents into the correlator, which is constructed such that the twist-3 LCDAs give dominant contribution and the twist-2 LCDAs make negligible contribution. Our results of the B → S transition form factors at the large recoil region q~2 ? 0 are consistent with those obtained in the literature, which inversely shows the present twist-3 LCDAs are acceptable.
机译:我们研究了标量介子a_0,K_0〜?的扭曲3的光锥分布幅度(LCDA)。 QCD和规则中的f_0和。通过在背景场方法的框架内对较大的s-夸克质量效应进行一致的处理,改进了QCD和规则。采用价夸克分量(-bar1q2)作为标量介子的主要结构,我们对其质量的估计接近于测得的a_0(1450),K_0〜?。 (1430)和f_0(1710)。从求和规则中,我们获得了扭曲3 LCDA的前两个非零力矩φ_(a_0)〜s,σ:〈ξ_(s,a_0)〜(2(4))〉 = 0.369(0.245)并且〈ξ_(σ,a_0)〜(24))〉 = 0.203(0.093);扭曲3 LCDAs的φ_(K_0〜?)〜(s,σ):〈ξ_(s,K_0〜?)〜(1(2))〉 = 0.004(0.355)和〈ξ_(σ,K_0〜 ?)〜(1(2))〉 = 0.018(0.207);以及扭曲3 LCDAs的φ_(f_0)〜(s,σ):〈ξ_(s,f_0)〜(2(4))〉 = 0.335(0.212)和〈ξ_(σ,f_0)〜(2 (4))> = 0.196(0.088)。作为这些Twist-3 LCDA的应用,我们通过向相关器中引入适当的手性电流来研究B→S跃迁的形状因数,其构造使得Twist-3 LCDA占主导地位而Twist-2 LCDA的贡献可忽略不计。我们在大反冲区域q〜2处的B→S过渡形状因子的结果。 0与文献中获得的一致,这反过来表明了目前的Twist-3 LCDA是可以接受的。

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