First inverse moment of the doubly-heavy baryon distribution amplitude from HQET sum rule

A. Shukhtina, Alexander Parkhomenko
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Abstract

Heavy-quark symmetry (HQS), despite being approximate, allows to relate dynamically many hadron systems. In the HQS-limit doubly-heavy baryons, whose dynamics is determined by a light quark situated in a color field of a static pair of heavy quarks, are similar to heavy mesons with a heavy antiquark. Non-local interpolation currents are introduced and corresponding matrix elements between the baryon and vacuum state are expressed in terms of light-cone distribution amplitudes. As well known, the first inverse moment of the leading twist -meson distribution amplitude (DA) is a very important hadronic parameter needed for an accurate theoretical description of -meson exclusive decays. It is quite natural that a similar moment of doubly-heavy baryons is of importance in exclusive doubly-heavy baryons’ decays. We obtain HQET sum rules for the first inverse moment based on the correlation functions containing nonlocal heavy-light operators of doubly-heavy baryons and their local interpolating currents.
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从HQET求和规则得到的重重子分布振幅的第一逆矩
重夸克对称(HQS),尽管是近似的,但允许动态地联系许多强子系统。在hqs极限中,双重重子的动力学是由位于静态重夸克对色场中的轻夸克决定的,它类似于带有重反夸克的重介子。引入非局域插值电流,用光锥分布幅值表示重子与真空态之间的矩阵元。众所周知,前导扭曲-介子分布振幅(DA)的第一逆矩是精确描述-介子独占衰变所需的一个非常重要的强子参数。很自然地,类似的重重子时刻在排他性重重子衰变中是重要的。基于包含双重重子非局部重-轻算子及其局部插值流的相关函数,得到了第一逆矩的HQET和规则。
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