Phases with modular ground states for symmetry breaking by rank 3 and rank 2 antisymmetric tensor scalars

Abstract

Working with explicit examples given by the 56 representation in $SU(8)$, and the 10 representation in $SU(5)$, we show that symmetry breaking of a group $\mathcal{G}\supset {\mathcal{G}}_1\times {\mathcal{G}}_2$ by a scalar in a rank three or two antisymmetric tensor representation leads to a number of distinct $modular$ ground states. For these broken symmetry phases, the ground state is periodic in an integer divisor $p$ of $N$, where $N>0$ is the absolute value of the nonzero $U(1)$ generator of the scalar component $\Phi$ that is a singlet under the simple subgroups ${\mathcal{G}}_1$ and ${\mathcal{G}}_2$. Ground state expectations of fractional powers ${\Phi }^{p/N}$ provide order parameters that distinguish the different phases. For the case of period $p=1$, this reduces to the usual Higgs mechanism, but for divisors $N\ge p>1$ of $N$ it leads to a modular ground state with periodicity $p$, implementing a discrete Abelian symmetry group $U(1)/Z_p$. This observation may allow new approaches to grand unification and family unification.

Latex, 13 pages. v3 substantially revised and expanded; v4, v5 have short additions to the text, with numbered equations the same as in v3

References in corpus (1)

• SU(8) family unification with boson-fermion balance

Cited by in corpus (2)

• $SU(n)$ symmetry breaking by rank three and rank two antisymmetric tensor scalars
• Further study of the maximally symmetry breaking patterns in an $\mathrm{SU}(8)$ theory