The equilibrium entropy of a small subsystem is ln d_A minus a 1/N^2 correction set by c^2 tr(X_A^2), where c and X_A are built from Hamiltonian moments and the initial energy spread.
High-precision simulation of finite-size thermalizing systems at long times
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abstract
To simulate thermalizing systems at long times, the most straightforward approach is to calculate the thermal properties at the corresponding energy. In a quantum many-body system of size $N$, for local observables and many initial states, this approach has an error of $O(1/N)$, which is reminiscent of the finite-size error of the equivalence of ensembles. In this paper, we propose a simple and efficient numerical method so that the simulation error is of higher order in $1/N$. This finite-size error scaling is proved by assuming the eigenstate thermalization hypothesis.
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Entropy of small subsystems in thermalizing systems
The equilibrium entropy of a small subsystem is ln d_A minus a 1/N^2 correction set by c^2 tr(X_A^2), where c and X_A are built from Hamiltonian moments and the initial energy spread.