Abstract
We put forward a simpler and improved variation of a recently proposed method to overcome the signal-to-noise problem found in Monte Carlo calculations of the entanglement entropy of interacting fermions. The present method takes advantage of the approximate lognormal distributions that characterize the signal-to-noise properties of other approaches. In addition, we show that a simple rewriting of the formalism allows circumvention of the inversion of the restricted one-body density matrix in the calculation of the -th Rényi entanglement entropy for . We test our technique by implementing it in combination with the hybrid Monte Carlo algorithm and calculating the Rényi entropies of the 1D attractive Hubbard model. We use that data to extrapolate to the von Neumann () and cases.
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