Polyakov loop model with exact static quark determinant in the 't Hooft-Veneziano limit: U(N) case
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arXiv
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| Format: | Preprint |
| Veröffentlicht: |
2025
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| _version_ | 1866917383310934016 |
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| author | Voloshyn, S. |
| author_facet | Voloshyn, S. |
| contents | I investigate a $d$-dimensional $U(N)$ Polyakov loop model that includes the exact static determinant with $N_f$ degenerate quark flavor and depends explicitly on the quark mass and chemical potential. In the large $N, N_f$ limit mean field gives the exact solution, and the core of the Polyakov loop model is reduced to a deformed unitary matrix model, which I solve exactly. I compute the free energy, the expectation value of the Polyakov loop, and the quark condensate. The phase diagram of the model and the type of phase transition is investigated and shows it depends on the ratio $κ=N_f/N$. |
| format | Preprint |
| id |
arxiv_https___arxiv_org_abs_2507_00689 |
| institution | arXiv |
| publishDate | 2025 |
| record_format | arxiv |
| spellingShingle | Polyakov loop model with exact static quark determinant in the 't Hooft-Veneziano limit: U(N) case Voloshyn, S. High Energy Physics - Lattice 81T25 (Primary) 81V05, 82B26 (Secondary) I investigate a $d$-dimensional $U(N)$ Polyakov loop model that includes the exact static determinant with $N_f$ degenerate quark flavor and depends explicitly on the quark mass and chemical potential. In the large $N, N_f$ limit mean field gives the exact solution, and the core of the Polyakov loop model is reduced to a deformed unitary matrix model, which I solve exactly. I compute the free energy, the expectation value of the Polyakov loop, and the quark condensate. The phase diagram of the model and the type of phase transition is investigated and shows it depends on the ratio $κ=N_f/N$. |
| title | Polyakov loop model with exact static quark determinant in the 't Hooft-Veneziano limit: U(N) case |
| topic | High Energy Physics - Lattice 81T25 (Primary) 81V05, 82B26 (Secondary) |
| url | https://arxiv.org/abs/2507.00689 |