It is shown that additional Bragg reflections can appear exclusively owing
to the local chirality associated with the left-right asymmetric environmen
t of scattering atoms in non-magnetic crystals. The structure amplitude of
these reflections depends on the antisymmetric part of a third-rank tensor
describing the spatial dispersion effects. It enhances for resonant near-ed
ge scattering through a mixed multipole transition, which includes a dipole
-quadrupole contribution. It is shown that this mechanism works even for ce
ntrosymmetric crystals, and some realistic examples are considered in detai
l (alpha -Fe2O3, LiNbO3 etc.). For instance, the interference between the d
ipole-quadrupole and quadrupole-quadrupole terms may be responsible for the
threefold symmetry of the azimuthal dependence of the hhh, h = 2n+1, refle
ctions observed recently in hematite.