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Five-Brane Superpotentials in Heterotic M-Theory

Eduardo Lima, Burt Ovrut, Jaemo Park

TL;DR

The paper computes a nonperturbative superpotential in heterotic M-theory arising from open membranes stretching between a boundary plane and a bulk five-brane. By performing a detailed κ-invariant construction, reducing to the heterotic string on a holomorphic curve, and evaluating the fermionic two-point function via a saddle-point expansion, it derives an explicit exponential suppression e^{−(T/2)𝔜} multiplied by determinants from bosonic, fermionic, and E8 boundary sectors. A key result is that the superpotential is holomorphic in the composite modulus 𝔜, built from the five-brane translation Y, the (1,1) modulus 𝒯 of the wrapped curve, and an axion, and it vanishes unless the boundary vector bundle restricts trivially to the curve. This provides a concrete mechanism for nonperturbative moduli stabilization and illuminates the role of boundary gauge bundles in controlling open-membrane instanton effects in heterotic M-theory.

Abstract

The open supermembrane contribution to the non-perturbative superpotential of bulk space five-branes in heterotic M-theory is presented. We explicitly compute the superpotential for the modulus associated with the separation of a bulk five-brane from an end-of-the-world three-brane. The gauge and kappa-invariant boundary strings of such open supermembranes are given and the role of the holomorphic vector bundle on the orbifold fixed plane boundary is discussed in detail.

Five-Brane Superpotentials in Heterotic M-Theory

TL;DR

The paper computes a nonperturbative superpotential in heterotic M-theory arising from open membranes stretching between a boundary plane and a bulk five-brane. By performing a detailed κ-invariant construction, reducing to the heterotic string on a holomorphic curve, and evaluating the fermionic two-point function via a saddle-point expansion, it derives an explicit exponential suppression e^{−(T/2)𝔜} multiplied by determinants from bosonic, fermionic, and E8 boundary sectors. A key result is that the superpotential is holomorphic in the composite modulus 𝔜, built from the five-brane translation Y, the (1,1) modulus 𝒯 of the wrapped curve, and an axion, and it vanishes unless the boundary vector bundle restricts trivially to the curve. This provides a concrete mechanism for nonperturbative moduli stabilization and illuminates the role of boundary gauge bundles in controlling open-membrane instanton effects in heterotic M-theory.

Abstract

The open supermembrane contribution to the non-perturbative superpotential of bulk space five-branes in heterotic M-theory is presented. We explicitly compute the superpotential for the modulus associated with the separation of a bulk five-brane from an end-of-the-world three-brane. The gauge and kappa-invariant boundary strings of such open supermembranes are given and the role of the holomorphic vector bundle on the orbifold fixed plane boundary is discussed in detail.

Paper Structure

This paper contains 9 sections, 316 equations.