Abstract

We study the bosonic matrix model obtained as the high-temperature limit of two-dimensional maximally supersymmetric SU(N) Yang-Mills theory. So far, no consensus about the order of the deconfinement transition in this theory has been reached and this hinders progress in understanding the nature of the black hole/black string topology change from the gauge/gravity duality perspective. On the one hand, previous works considered the deconfinement transition consistent with two transitions which are of second and third order. On the other hand, evidence for a first order transition was put forward more recently. We perform high-statistics lattice Monte Carlo simulations at large N and small lattice spacing to establish that the transition is really of first order. Our findings flag a warning that the required large-N and continuum limit might not have been reached in earlier publications, and that was the source of the discrepancy. Moreover, our detailed results confirm the existence of a new partially deconfined phase which describes non-uniform black strings via the gauge/gravity duality. This phase exhibits universal features already predicted in quantum field theory.

Highlights

  • Defined by DtXI = ∂tXI − i[At, XI ], where At is the gauge field

  • The bosonic matrix model is obtained by shrinking the temporal circle of the two-dimensional supersymmetric Yang-Mills (SYM) theory to a point

  • The phase transition we study in this paper is the remnant of center symmetry breaking/restoration along the spatial S1 in this higher-dimensional theory, which can be regarded as the black hole/black string topology change in the R1,8 × S1 spacetime of the dual gravitational description [9]

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Summary

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The phase transition we study in this paper is the remnant of center symmetry breaking/restoration along the spatial S1 in this higher-dimensional theory, which can be regarded as the black hole/black string topology change in the R1,8 × S1 spacetime of the dual gravitational description [9]. The study did not consider discretisation effects which may affect the nature of the transition by shuffling the order of temperatures if there are multiple transitions as expected from the large-D analysis (see figure 3) This was due to the limited computational resources available to deal with the considerable increase in numerical cost for larger N and smaller lattice spacing.

Theoretical expectations
Partial deconfinement and possible phase structures
Finite-N effects
The order of the phase transition and the large-D limit
First order signals from other observables
Partial deconfinement
Conclusion and future directions
A Simulation details
Full Text
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