Partial deconfinement in QCD at $N=3$ and $N=\infty$

We describe how the general mechanism of partial deconfinement applies to large- $N$ QCD and the partially-deconfined phase inevitably appears between completely-confined and completely-deconfined phases. Furthermore, we propose how the partial deconfinement can be observed in the real-world QCD with SU(3) gauge group. We propose the relationship between the behaviors of the Polyakov loop and other quantities. We test our proposal against lattice simulation data and find a nontrivial matching.

Partial deconfinement in QCD at $N = 3$ and $N = \infty$

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Partial deconfinement in QCD at $N = 3$ and $N = \infty$

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Partial deconfinement in QCD at N=3N=3 and N=∞N=∞

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Partial deconfinement in QCD at N=3N=3 and N=∞N=∞

文献摘要

讨论

|讲解博客

|AI智能校验

Partial deconfinement in QCD at $N = 3$ and $N = \infty$

讲解博客

AI智能校验

Partial deconfinement in QCD at $N = 3$ and $N = \infty$

讲解博客

AI智能校验