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We consider a class of Hubbard-Stratonovich transformations suitable for treating Hubbard interactions in the context of quantum Monte Carlo simulations. A tunable parameter allows us to continuously vary from a discrete Ising auxiliary field () to a compact auxiliary field that couples to electrons sinusoidally (). In tests on the single-band Hubbard model, we find that the severity of the sign problem decreases systematically with increasing . Selecting finite, however, enables continuous sampling methods like the Langevin or Hamiltonian Monte Carlo methods. We explore the tradeoffs between various simulation methods through numerical benchmarks.

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