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Nonperturbative correlation functions from homotopy algebras

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arxiv 2405.10935 v3 pith:UCA4V6ZZ submitted 2024-05-17 hep-th

classification hep-th
keywords functionscorrelationformulatheoryalgebrasarxivlefschetzsolution
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abstract

The formula for correlation functions based on quantum $A_\infty$ algebras in arXiv:2203.05366, arXiv:2305.11634, and arXiv:2305.13103 requires us to divide the action into the free part and the interaction part. We present a new form of the formula which does not involve such division. The new formula requires us to choose a solution to the equations of motion which does not have to be real, and we claim that the formula gives correlation functions evaluated on the Lefschetz thimble associated with the solution we chose. Our formula correctly reproduces correlation functions in perturbation theory, but it can be valid nonperturbatively, and we present numerical evidence for scalar field theories in zero dimensions both in the Euclidean case and the Lorentzian case that correlation functions for finite coupling constants can be reproduced. When the theory consists of a single Lefschetz thimble, our formula gives correlation functions of the theory by choosing the solution corresponding to the thimble. When the theory consists of multiple Lefschetz thimbles, we need to evaluate the ratios of the partition functions for those thimbles and we describe a method of such evaluations based on quantum $A_\infty$ algebras in a forthcoming paper.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. The BEF Symplectic Form: A Lagrangian Perspective

    hep-th 2026-04 unverdicted novelty 7.0 of 10

    The BEF symplectic form is derived from L∞-Lagrangians via covariant phase space methods and coincides with the Barnich-Brandt form for second-order equations of motion.

  2. Universal quadratic field equations via homotopy algebras

    hep-th 2026-08 conditional novelty 6.0 of 10

    The bar-cobar construction turns the equations of motion of any homotopy-algebra gauge theory into universal quadratic Maurer-Cartan equations, with solutions equivalent to the original theory.

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