I discuss a method to define a theta-angle in 1+1D gauge theories with matter in a way which allows for a dual description without the sign problem. The method begins with non-compact gauge theory with a continuous R-valued center symmetry. By gauging the center symmetry down to U(1), a natural theta-term can be introduced through the gauge field for the center symmetry. The theory in this formulation can be dualized in such a way so that the sign problem is avoided. I discuss briefly the special case of theta=pi and possible scenarios that can be tested in lattice simulations.

Theoretical Developments