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Physical meaning of complex-coupling integrating-out in topological strings

Determine the physical interpretation of the M-theory integrating-out procedure for BPS M2-brane states, formulated via Schwinger proper-time integrals and contour deformations, when the topological string coupling λ is complex (λ = λr + iλi), and ascertain whether the associated pole-crossing Stokes jumps and non-perturbative contributions represent physically correct features of the topological string free energy.

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Background

The paper proposes an exact integrating-out formula for the holomorphic-limit, non-perturbative topological string free energy based on M2-brane BPS states and evaluates it through contour integrals in complexified Schwinger proper time. For real coupling λ, the analysis identifies perturbative and non-perturbative poles and matches known non-perturbative completions in specific cases.

When λ is extended to complex values, the non-perturbative poles rotate in the complex plane and may cross integration rays, producing additional contour contributions interpreted as Stokes jumps. Although mathematically well-defined within the proposed framework, the authors state that the physical meaning of the integrating-out calculation for complex λ, and the physical validity of the resulting properties (including the Stokes jumps), is not clear and requires further investigation.

References

While complex $\lambda$ manifests some interesting properties, physically it is not clear what the integrating out calculation means for complex $\lambda$, and so it is not clear that these properties are really physically correct. We leave a better understanding of complex $\lambda$ physics for future work.

Non-perturbative topological string theory on compact Calabi-Yau manifolds from M-theory (2408.09255 - Hattab et al., 17 Aug 2024) in Section 3 (Pole crossing jumps)