Recent neutron scattering [1,2], and optical measurements [3,4] have detected evidence in underdoped cuprate superconductors for a phase transition near the pseudogap onset temperature T * to a time reversal-breaking state. The neutron scattering indicates antiferromagnetic ordering, while it is often assumed that optical polarization rotation requires at least a weak ferromagnetic component. In this note we identify several antiferromagnetic structures, compatible with neutron scattering data, that allow intrinsic polarization rotation through the magnetoelectic effect.1 High-T c superconductivity in the cuprates remains a controversial field after more than 20 years of intense research [5]. One of the few ideas that has achieved broad consensus is that solving the puzzle of high-T c requires first understanding the normal phase from which it evolves. Early in the study of these materials, various probes, particularly thermodynamic ones, failed to detect a phase transition above the critical temperature for superconductivity.Instead, the most prominent feature of the normal state is the loss with decreasing temperature of states at the Fermi energy -the pseudogap phenomenon [6]. The lack of evidence for a phase transition suggested that the opening of the pseudogap reflects a crossover, rather than the appearance of a new phase with a distinct symmetry. Subsequently, careful experiments revealed that in certain cuprates, at doping levels close to 1/8, there were indeed phase transitions to states with true charge and spin density order [7]. Thus the possibility exists that proximity to these translational symmetry breaking phases controls the physics in cuprates that do not manifest this form of static order. Kerr rotation is a direct manifestation of broken time-reversal, and therefore its appearance tends to support the neutron scattering findings. Although the experiments have yet to be