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arXiv 1503.02719hep-ph
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$X(3872) \to χ_{cJ} π^0$的EFT计算中的强子环与因子分解

Hadronic Loops versus Factorization in EFT calculations of $X(3872) \to χ_{cJ} π^0$

Thomas Mehen

摘要:

以$X(3872) \to χ_{cJ} π^0$为例,比较了有效场论中两种计算分子夸克偶素态到常规夸克偶素衰变的方法。在一种方法中,分子夸克偶素的衰变通过一个三角图进行,环中有粲介子。我们认为,这种方法预测过大的$Γ[X(3872) \to χ_{cJ}π^0]$率,除非带电和中性介子都包括在内,这些贡献之间的取消安排,以抑制衰变率。如果$X(3872)$主要在$I=0$ $D \bar{D}^{*} +c.c.$散射信道中,则这种抵消自然发生。分子衰变的因式分解方法计算了$X(3872)$中$D$介子到最终态的树能级跃迁的速率,乘以未知的矩阵元素。我们表明,这种方法是等价于强子回路的方法,如果截止的回路积分是几百MeV或更小,是适当的,当带电$D$介子已被整合出XEFT。

英文摘要:

We compare two existing approaches to calculating the decay of molecular quarkonium states to conventional quarkonia in effective field theory, using $X(3872) \to χ_{cJ} π^0$ as an example. In one approach the decay of the molecular quarkonium proceeds through a triangle diagram with charmed mesons in the loop. We argue this approach predicts excessively large rates for $Γ[X(3872) \to χ_{cJ}π^0]$ unless both charged and neutral mesons are included and a cancellation between these contributions is arranged to suppress the decay rates. This cancellation occurs naturally if the $X(3872)$ is primarily in the $I=0$ $D \bar{D}^{*} +c.c.$ scattering channel. The factorization approach to molecular decays calculates the rates in terms of tree-level transitions for the $D$ mesons in the $X(3872)$ to the final state, multiplied by unknown matrix elements. We show that this approach is equivalent to hadronic loops approach if the cutoff on the loop integrations is taken to be a few hundred MeV or smaller, as is appropriate when the charged $D$ mesons have been integrated out of XEFT.

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