Using the finite size scaling theory, we reexamine the nature of the bulk phase transition in the fundamental-adjoint coupling plane of the SU(2) lattice gauge theory at beta(A) = 1.25 where previous finite size scaling investigations of the deconfinement phase transition showed it to be of first order for temporal lattices with four sites. Our simulations on N-4 lattices with N = 6, 8, 10, 12 and 16 show an absence of a first order bulk phase transition. We find the discontinuity in the average plaquette to decrease approximately linearly with N. Correspondingly, the plaquette susceptibility grows a lot slower with the 4-volume of the lattice than expected from a first order bulk phase transition.
机构:
Inst High Energy Phys, Protvino 142280, Moskovskaya Obl, Russia
Inst Theoret & Expt Phys, Moscow 117218, RussiaInst High Energy Phys, Protvino 142280, Moskovskaya Obl, Russia
Bornyakov, V. G.
Kononenko, A. G.
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Moscow MV Lomonosov State Univ, Dept Phys, Moscow 119991, RussiaInst High Energy Phys, Protvino 142280, Moskovskaya Obl, Russia