Antisymmetric tensor Z_p gauge symmetries in field theory and string theory

Understand

We consider discrete gauge symmetries in D dimensions arising as remnants of broken continuous gauge symmetries carried by general antisymmetric tensor fields, rather than by standard 1-forms.

• The lagrangian for such a general ${\bf Z}_p$ gauge theory can be described in terms of a $r$-form gauge field made massive by a $(r-1)$-form, or other dual realizations, that we also discuss.
• The theory contains charged topological defects of different dimensionalities, generalizing the familiar charged particles and strings in D=4.
• We describe realizations in string theory compactifications with torsion cycles, or with background field strength fluxes.