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Updated: Jun 22, 2025

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Setting Limits on Supersymmetry Using Simplified Models
Published on: November 15, 2013
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从格子QCD的合通道散射中的标量和张量共振
David J Wilson1, Christopher E Thomas1, Jozef J Dudek2,3
1DAMTP, University of Cambridge, Centre for Mathematical Sciences, Wilberforce Road, Cambridge CB3 0WA, United Kingdom.
Physical review letters
|July 1, 2024
概括
格子QCD计算显示了单个 χ_{c0} 和 χ_{c2} 共振在区域. 这些在4000 MeV以下的共振,显示出与开放性魅惑性介子通道的显著合.
科学领域:
- * 核和粒子物理学.
- * 量子染色动力学 (QCD).
背景情况:
- * 了解子光谱和相互作用对于粒子物理学至关重要.
- * 之前的理论和实验研究表明,在频谱中存在不同的共振结构.
研究的目的:
- * 通过使用格子QCD在充能量区域中确定哈德龙-哈德龙散射幅度.
- * 在这个能量范围内识别和描述共振,特别是 χ_{c0} 和 χ_{c2} .
主要方法:
- * 采用格子QCD,这是量子染色动力学的第一原则方法.
- * 在特定的 pion 质量 (m_{π}≈391 MeV) 上计算超过 200 个有限体积能量水平.
- *利用Lüscher形式主义的扩展来导出无限体积的散射幅度.
主要成果:
- * 确定了一个单一的 χ_{c0} 和一个单一的 χ_{c2} 反响,出现在4000 MeV以下的极点奇点中.
- * 确定共振宽度大约为70 MeV.
- * 发现了与动力关闭的D*D*通道和各种开放的魅力中子衰变通道的大而重要的合.
结论:
- *高达4100 MeV的碳能量区域包含一个单一的 χ_{c0} 和 χ_{c2} 共振.
- *这些发现与一些先前的理论和实验预测相反,这些预测涉及到标量束状态和接近值的共振.
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