Bulk-Brane Duality in Field Theory

TL;DR

This paper explores a controllable bulk-brane duality in a supersymmetric field theory by compactifying one spatial dimension, mapping 4D bulk dynamics onto a 3D boundary theory, and analyzing quantum effects on domain walls.

Contribution

It demonstrates a novel bulk-brane duality in field theory using a compactified setup, linking 4D and 3D supersymmetric theories with controlled parameters.

Findings

Mapping of 4D bulk dynamics to 3D boundary theory.

Generation of a Chern-Simons term on the wall.

Mass gap development for excitations on the walls.

Abstract

We consider (3+1)-dimensional N=2 supersymmetric QED with two flavors of fundamental hypermultiplets. This theory supports 1/2-BPS domain walls and flux tubes (strings), as well as their 1/4-BPS junctions. The effective (2+1)-dimensional theory on the domain wall is known to be a U(1) gauge theory. Previously, the wall-string junctions were shown to play the role of massive charges in this theory. However, the field theory of the junctions on the wall (for semi-infinite strings) appears to be inconsistent due to infrared problems. All these problems can be eliminated by compactifying one spatial dimension orthogonal to the wall and considering a wall-antiwall system on a cylinder. We argue that for certain values of parameters this set-up provides an example of a controllable bulk-brane duality in field theory. Dynamics of the 4D bulk are mapped onto 3D boundary theory: 3D N=2 SQED with two matter superfields and a weak-strong coupling constant relation in 4D and 3D, respectively. The cylinder radius is seen as a "real mass" in 3D N=2 SQED. We work out (at weak coupling) the quantum version of the world-volume theory on the walls. Integrating out massive matter (strings in the bulk theory) one generates a Chern-Simons term on the wall world volume and an interaction between the wall and antiwall that scales as a power of distance. Vector and scalar (classically) massless excitations on the walls develop a mass gap at the quantum level; the long-range interactions disappear. The above duality implies that the wall and its antiwall partner (at strong coupling in the bulk theory) are stabilized at the opposite sides of the cylinder.