Lattice Scalar Field Theory At Complex Coupling

Abstract

Lattice scalar field theories encounter a sign problem when the coupling constant is complex. This is a close cousin of the real-time sign problems that afflict the lattice Schwinger-Keldysh formalism, and a more distant relative of the fermion sign problem that plagues calculations of QCD at finite density. We demonstrate the methods of complex normalizing flows and contour deformations on scalar fields in $0+1$ and $1+1$ dimensions, respectively. In both cases, intractable sign problems are readily bypassed. These methods extend to negative couplings, where the partition function can be defined only by analytic continuation. Finally, we examine the location of partition function zeros, and discuss their relation to the performance of these algorithms.

9 pages, 6 figures

References in corpus (3)

• Structure of Lefschetz thimbles in simple fermionic systems
• Schwinger-Keldysh on the lattice: a faster algorithm and its application to field theory
• Deep Learning Beyond Lefschetz Thimbles

Cited by in corpus (6)

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• Convex optimization and contour deformations