The
self-consistent coupled-perturbed (SC-CP) method in the CRYSTAL
program has been adapted to obtain electromagnetic optical rotation
properties of chiral periodic systems based on the calculation of
the magnetic moment induced by the electric field. Toward that end,
an expression for the magnetic transition moment is developed, which
involves an appropriate electronic angular momentum operator. This
operator is forced to be hermitian so that the chiroptical properties
are real. In our formulation, the trace of the optical rotatory power
matrix is gauge-origin-invariant as long as the electric dipole transition
matrix elements are obtained using the velocity (rather than position)
operator. On the other hand, the component along the optic axis is
invariant in general for uniaxial and biaxial crystals. Under the
same conditions, these properties also do not depend on the so-called
missing integers that occur in the treatment of the electric dipole
moment of quasi-one-dimensional periodic systems or the analogue of
missing integers for the case of higher dimensionality. Tests on a
model H2O2 polymer confirm the formalism and,
as desired, show that the calculated properties are independent of
the size and definition of the unit cell. In addition, an empirical
relation to a finite oligomer gauge-including atomic orbital (GIAO)
calculation is found. Applications, with comparison to experiment,
are carried for α-quartz, tartaric acid crystal, and carbon
nanotubes. Future developments of this initial approach to chiroptical
properties in the solid state are noted.