θ dependence of Tc in SU(2) Yang-Mills theory

A bstract We present an exploratory study to determine the confinement-deconfinement transition temperature at finite θ , T c ( θ ), for the 4d SU(2) pure Yang-Mills theory. Lattice numerical simulations are performed on three spatial sizes N S = 24, 32, 48 with a fixed temporal size N T = 8. We introduce a non-zero θ -angle by the sub-volume method to mitigate the sign problem. By taking advantage of the universality in the second order phase transition and the Binder cumulant of the order parameter, the θ -dependence of T c is determined to be T c ( θ )/ T c (0) = 1 − 0 . 16(2) ( θ / π ) 2 − 0 . 03(4) ( θ / π ) 4 up to θ ∼ 0.9 π . The reliability of the extrapolations in the sub-volume method is extensively checked. We also point out that the temperature dependence of the topological susceptibility should exhibit a singularity with the exponent for the specific heat.

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Publication Details

Journal
Journal of High Energy Physics
Published
2025-02-28
DOI
https://doi.org/10.1007/jhep02(2025)211
Citations
3
Primary Topic
Quantum Chromodynamics and Particle Interactions
Type
article
Field-Weighted Citation Impact
5.61
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article

θ dependence of Tc in SU(2) Yang-Mills theory

N. Yamada, Ryuichiro Kitano, Masahito Yamazaki
3 citations
Journal of High Energy Physics
Quantum Chromodynamics and Particle Interactions
5.61
article

θ dependence of Tc in SU(2) Yang-Mills theory

N. Yamada, Ryuichiro Kitano, Masahito Yamazaki
article en
3 citations

Abstract

A bstract We present an exploratory study to determine the confinement-deconfinement transition temperature at finite θ , T c ( θ ), for the 4d SU(2) pure Yang-Mills theory. Lattice numerical simulations are performed on three spatial sizes N S = 24, 32, 48 with a fixed temporal size N T = 8. We introduce a non-zero θ -angle by the sub-volume method to mitigate the sign problem. By taking advantage of the universality in the second order phase transition and the Binder cumulant of the order parameter, the θ -dependence of T c is determined to be T c ( θ )/ T c (0) = 1 − 0 . 16(2) ( θ / π ) 2 − 0 . 03(4) ( θ / π ) 4 up to θ ∼ 0.9 π . The reliability of the extrapolations in the sub-volume method is extensively checked. We also point out that the temperature dependence of the topological susceptibility should exhibit a singularity with the exponent for the specific heat.

Journal of High Energy PhysicsVol. 2025(2)
High Energy Accelerator Research Organization (JP), Kavli Institute for the Physics and Mathematics of the Universe (JP), The Graduate University for Advanced Studies, SOKENDAI (JP), The University of Tokyo (JP)
Openalex Percentile: Top 5%
Quantum Chromodynamics and Particle Interactions
5.61
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