Clash of symmetries on the brane

TL;DR

This paper introduces the "clash of symmetries" phenomenon in brane-world models, where different embeddings of symmetry subgroups lead to novel symmetry breaking patterns on domain walls, with potential implications for grand unified theories.

Contribution

It presents a new mechanism of symmetry breaking via domain wall solutions connecting vacua with differently embedded subgroups, illustrated with a three-Higgs-triplet toy model.

Findings

Demonstrates symmetry breaking to subgroup intersections on domain walls.

Constructs a three-fold domain wall junction with symmetric vacuum portions.

Discusses potential links to E6 grand unification.

Abstract

If our 3+1-dimensional universe is a brane or domain wall embedded in a higher dimensional space, then a phenomenon we term the ``clash of symmetries'' provides a new method of breaking some continuous symmetries. A global $G_{\text{cts}} \otimes G_{\text{discrete}}$ symmetry is spontaneously broken to $H_{\text{cts}} \otimes H_{\text{discrete}}$, where the continuous subgroup $H_{\text{cts}}$ can be embedded in several different ways in the parent group $G_{\text{cts}}$, and $H_{\text{discrete}} < G_{\text{discrete}}$. A certain class of topological domain wall solutions connect two vacua that are invariant under {\it differently embedded} $H_{\text{cts}}$ subgroups. There is then enhanced symmetry breakdown to the intersection of these two subgroups on the domain wall. This is the ``clash''. In the brane limit, we obtain a configuration with $H_{\text{cts}}$ symmetries in the bulk but the smaller intersection symmetry on the brane itself. We illustrate this idea using a permutation symmetric three-Higgs-triplet toy model exploiting the distinct $I-$, $U-$ and $V-$spin U(2) subgroups of U(3). The three disconnected portions of the vacuum manifold can be treated symmetrically through the construction of a three-fold planar domain wall junction configuration, with our universe at the nexus. A possible connection with $E_6$ is discussed.