Determine the twisted-boundary-condition three-loop coefficient

Determine the analytic form of the three-loop coefficient \(\beta(\eta)\) for the bosonic membrane on \(\mathbb{R}^2\times S^1\) with twist parameter \(\eta\), including its dependence on single-valued polylogarithms or level-two Euler sums, and thereby complete the three-loop result for twisted boundary conditions.

Background

For twisted boundary conditions, the ordinary ζ(3)\zeta(3) factors in the three-loop six-vertex and chain contributions are replaced by a twist-dependent function Φ(η)\Phi(\eta). The remaining basketball contribution is governed by a coefficient β(η)\beta(\eta).

The untwisted value β(0)\beta(0) is conjecturally expressed in terms of ζ(9)\zeta(9) and ζ(3)3\zeta(3)^3, while the antiperiodic value involves constants outside the ordinary weight-nine basis because the twist mixes periods and generates level-two Euler sums. The paper leaves the general analytic form of β(η)\beta(\eta) unresolved, suggesting an ansatz in terms of single-valued polylogarithms.

References

For twisted boundary conditions the factors of \zeta(3) in #1{513} and #1{6vc} should be replaced by \Phi(\eta) defined in #1{c5}, but we did not manage to find the corresponding guess for \beta(\eta) in #1{5231},#1{clos}. The above analogy with single-valued zeta's suggests a natural ansatz.

Energy of toroidal M2 brane in flat 11d background  (2608.23517 - Tseytlin et al., 24 Aug 2026) in Section 5, subsection “Membrane on \(\mathbb R^2\times\tilde S^1\),” final discussion of twisted boundary conditions