Diffraction of helical x-rays by optically active achiral crystals
Stephen W. Lovesey

TL;DR
This paper investigates how optically active achiral crystals produce unique diffraction patterns with circularly polarized x-rays, revealing chiral signatures linked to electron distribution and resonance effects, enhancing understanding of Templeton-Templeton scattering.
Contribution
It provides a detailed analysis of chiral diffraction signatures in optically active achiral crystals using resonant x-ray scattering, including electric dipole interactions and resonance enhancement effects.
Findings
Resonant x-ray tuning amplifies weak Templeton-Templeton scattering signals.
Chiral signatures depend on crystal symmetry, Wyckoff positions, and azimuthal angle.
Space-group forbidden spots become element-specific at resonance.
Abstract
Four crystal classes are optically active yet not chiral (non-enantiomorphic). Corresponding Bragg diffraction patterns calculated for circularly polarized (helical) x-rays tuned to an atomic resonance prove that angular anisotropy in the distribution of electrons create spots not indexed on the chemical structure (defined by a space group derived from Thomson scattering by perfect spheres of charge). Templeton-Templeton scattering, as it is usually called, of helical x-rays is quantified in terms of a chiral signature defined as the partial diffracted intensity hallmarked by x-ray helicity. Our electric dipole - electric dipole (E1-E1) chiral signature for a space group in the optically active crystal class D2d affords a complete interpretation in terms of copper quadrupoles of diffraction data collected on copper metaborate [E. N. Ovchinnikova et al., J. Synchrotron Rad. 28, 1455…
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