Deconfinement transition and string tensions in SU(4) Yang-Mills Theory

Physics – High Energy Physics – High Energy Physics - Lattice

Scientific paper

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10 pages with included figures. For version 2: New calculation and discussion of latent heat added; 2 new figures and 1 new ta

Scientific paper

10.1103/PhysRevD.63.094502

We present results from numerical lattice calculations of SU(4) Yang-Mills theory. This work has two goals: to determine the order of the finite temperature deconfinement transition on an $N_t = 6$ lattice and to study the string tensions between static charges in the irreducible representations of SU(4). Motivated by Pisarski and Tytgat's argument that a second-order SU($\infty$) deconfinement transition would explain some features of the SU(3) and QCD transitions, we confirm older results on a coarser, $N_t = 4$, lattice. We see a clear two-phase coexistence signal, characteristic of a first-order transition, at $8/g^2 = 10.79$ on a $6\times 20^3$ lattice, on which we also compute a latent heat of $\Delta\epsilon\approx 0.6 \epsilon_{SB}$. Computing Polyakov loop correlation functions we calculate the string tension at finite temperature in the confined phase between fundamental charges, $\sigma_1$, between diquark charges, $\sigma_2$, and between adjoint charges $\sigma_4$. We find that $1 < \sigma_2/\sigma_1 < 2$, and our result for the adjoint string tension $\sigma_4$ is consistent with string breaking.

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