The Manakov-Zakharov-Ward model as an integrable decoupling limit of the membrane
David Osten
TL;DR
The paper introduces a novel decoupling limit of the bosonic membrane in a toroidal background that yields the $(1+2)$-dimensional Manakov-Zakharov-Ward (MZW) integrable model. This regime arises from a large-wrapping limit combined with a non-Lorentzian scaling of the background, and can be embedded into the eleven-dimensional uplift of AdS$_3\times$S$^3\times$T$^4$. In the transverse sector, the membrane dynamics reduce to the MZW sigma-model with current $j=g^{-1}dg$, obeying the MZW equations and admitting a Lax structure and infinite conserved charges, thereby providing a physical realization of a higher-dimensional integrable theory. The work opens avenues for exploring non-Lorentzian membrane limits, interpreting conserved charges in this context, and connecting to holographic setups and higher Chern–Simons theories to discover further integrable regimes in membrane dynamics.
Abstract
A novel decoupling limit of the membrane is proposed, leading to the $(1+2)$-dimensional classically integrable model originally introduced by Manakov, Zakharov, and Ward. This limit is the large-wrapping regime of a membrane propagating toy background of the form $\mathbb{R}_t \times T^2 \times G$ subject to scaling limit, where $G$ is a Lie group and the geometry is supported by a four-form flux. Such toy backgrounds can arise from consistent eleven-dimensional supergravity solutions, exemplified by the uplift of the pure NSNS AdS$_3 \times$ S$^3 \times$ T$^4$ background. The scaling limit can be interpreted as similtaneous small tension and non- or hyper-relativistic limit.
