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arXiv 2602.15097hep-thhep-lathep-ph
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渐近自由对束缚弦的印记

Imprints of asymptotic freedom on confining strings

Princeton University(普林斯顿大学);University of California, Santa Barbara(加州大学圣塔芭芭拉分校);Caltech(加州理工学院)

Jan Albert, Alexandre Homrich

AI总结:

研究通过分析大N杨-米尔斯理论中束缚弦的渐近谱密度,揭示了弱耦合紫外部分与高能磁通管动力学的联系,并限制了Goldstone模的散射数据。

摘要:

我们考虑了大N杨-米尔斯理论在三维和四维 confinement 相中的 Polyakov 回转相关子。它可以通过求和封闭磁通管绕热循环缠绕的交换来计算。在短距离下,主导的发散由微扰理论控制。结合这两个事实,我们可以确定贡献于相关子的弦态的渐近谱密度。这清晰地将弱耦合的紫外部分与高能磁通管的动力学联系起来。然后,在一个玩具可积设定中,我们探讨如何通过长弦上的 Goldstone 模式的散射数据来限制这一情况。我们推导了一个关于 Goldstone 对磁通管边界反射振幅渐近行为的限制,并排除了 S 矩阵的渐近线性相移。在过程中,我们讨论了因果性如何对热力学量施加限制,并展示了时间延迟的正性如何从二维无质量弹性 S 矩阵的单位性和解析性得出。我们还包含了一个关于反射振幅的综述,以及在长有效弦理论中其计算的综述。

英文摘要:

We consider the Polyakov loop correlator in the confining phase of large $N$ Yang-Mills theory in three and four dimensions. It can be computed by summing over the exchange of closed flux tubes winding around the thermal cycle. At short separations, the leading divergence is controlled by perturbation theory. Combining these two facts allows us to determine the asymptotic spectral density of string states contributing to the correlator. This sharply relates the weakly-coupled UV of the gauge theory to the dynamics of highly energetic flux tubes. Then, in a toy integrable setting, we explore how this can bound the scattering data of the Goldstone modes on top of a long string. We derive a bound on the asymptotic behavior of the reflection amplitude of Goldstones against the flux tube boundary sourced by the Polyakov line, and rule out an asymptotically linear phase shift for the S-matrix. Along the way, we discuss how causality can impose bounds on thermodynamic quantities, and show how the positivity of time delays follows from unitarity and analyticity of $2d$ massless elastic S-matrices. We include a review on reflection amplitudes, and their computation in the theory of long effective strings.

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