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arXiv 2609.04628hep-ph

隐藏奇异$1^{++}$四夸克质量与径向激发的QCD求和规则分析

QCD sum rule analysis of hidden strange $1^{++}$ tetraquark masses and radial excitations

  • Jishou University(吉首大学)
  • Sun Yat-Sen University(中山大学)
  • Institute of Modern Physics, Chinese Academy of Sciences(中国科学院近代物理研究所)
  • Dordt University(多德大学)

机构由 AI 辅助整理,请以论文原文为准。

Zhuo-Ran Huang, Wei Chen, Jason Ho, Lei-Hua Liu

AI总结:

本文通过QCD求和规则分析隐藏奇异$1^{++}$四夸克,确定$us\bar{u}\bar{s}$基态质量,发现$a_1(1930)$是致密$1^{++}$四夸克候选者,并讨论其可在未来实验检验的衰变道。

AI中文摘要:

我们利用QCD求和规则重新研究具有量子数$J^{PC}=1^{++}$的轻四夸克态,重点关注一组完整的无导数双夸克-反双夸克插值流。通过计算维度8凝聚态的算符乘积展开,我们从拉普拉斯求和规则(LSR)和有限能量求和规则(FESR)中提取了隐藏奇异$us\bar{u}\bar{s}$四夸克的基态质量,联合分析得到$M_{us\bar{u}\bar{s}} = 1.45\tilde{+}0.11$ GeV,该结果与$a_1(1420)$共振的质量吻合良好,支持其四夸克解释。此外,我们采用双共振窄宽度模型进行高斯求和规则(GSR)分析以探测径向激发,GSR拟合揭示了一个质量为$m_2 = 1.86\tilde{+}0.12$ GeV的较重态,以及较轻态的相对耦合$r = 0.15\tilde{+}0.03$,表明$a_1(1930)$是致密$1^{++}$四夸克的有希望候选者。我们还讨论了这些四夸克候选者的主导衰变模式,强调了$K^*K$和$f_0(980)\pi$等隐藏奇异道,这些可在未来实验中进行检验。

英文摘要:

We revisit the light tetraquark states with quantum numbers $J^{PC}=1^{++}$ using QCD sum rules, focusing on a complete set of derivative-free diquark-antidiquark interpolating currents. By calculating the operator product expansion up to dimension-eight condensates, we extract the ground-state mass of the hidden-strange $us\bar{u}\bar{s}$ tetraquark from both Laplace sum rules (LSR) and finite-energy sum rules (FESR). Our combined analysis yields $M_{us\bar{u}\bar{s}} = 1.45\pm0.11$~GeV, which agrees well with the mass of the $a_1(1420)$ resonance and supports its tetraquark interpretation. Furthermore, we perform Gaussian sum rule (GSR) analyses to probe radial excitations, adopting a two-resonance narrow-width model. The GSR fit reveals a heavier state with mass $m_2 = 1.86\pm0.12$~GeV and a relative coupling $r = 0.15\pm0.03$ for the lighter state, indicating that the $a_1(1930)$ is a promising candidate for a compact $1^{++}$ tetraquark. We also discuss the dominant decay modes of these tetraquark candidates, emphasizing hidden-strange channels such as $K^*K$ and $f_0(980)π$, which can be tested in future experiments.

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