12.4 CHIRAL INTERMEDIATE-PERIOD GRATING
12.4.1 Symmetry of CIPG Structures
We next consider the differences between propagation in a planar and in a fiber
geometry. Because the sample is no longer uniform in the transverse direction,
core modes may be scattered into modes with propagation vector pointing away
from the fiber axis when the difference between the propagation constant of the
core mode and the scattered wave is compensated by the grating constant associated
with the periodic structure. In FBGs, the forward and backwards propagating core
modes are coupled via the grating constant, which is 2p=a, where a is the grating
period. In chiral fibers, core modes are similarly coupled via the grating condition
above. In single-helix chiral gratings ...