Abstract

We study the maximally supersymmetric BFSS model at finite temperature and its bosonic relative. For the bosonic model in p+1p+1 dimensions, we find that it effectively reduces to a system of gauged Gaussian matrix models. The effective model captures the low temperature regime of the model including one of its two phase transitions. The mass becomes p1/3λ1/3p^{1/3}λ^{1/3} for large pp, with λλ the 'tHooft coupling. Simulations of the bosonic-BFSS model with p=9p=9 give m=(1.965±.007)λ1/3m=(1.965\pm .007)λ^{1/3}, which is also the mass gap of the Hamiltonian. We argue that there is no `sign' problem in the maximally supersymmetric BFSS model and perform detailed simulations of several observables finding excellent agreement with AdS/CFT predictions when 1/α′1/α' corrections are included.

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