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High-pressure polymorphism in l -threonine between ambient pressure and 22 GPa
- Giordano, Nico;
- Beavers, Christine M;
- Kamenev, Konstantin V;
- Marshall, William G;
- Moggach, Stephen A;
- Patterson, Simon D;
- Teat, Simon J;
- Warren, John E;
- Wood, Peter A;
- Parsons, Simon
Published Web Location
https://doi.org/10.1039/c9ce00388fAbstract
The amino acid l -threonine undergoes three phase transitions between ambient pressure and 22.3 GPa which modify both hydrogen bonding and the molecular conformation.
The crystal structure of l -threonine has been studied to a maximum pressure of 22.3 GPa using single-crystal X-ray and neutron powder diffraction. The data have been interpreted in the light of previous Raman spectroscopic data by Holanda et al. ( J. Mol. Struct. (2015), 1092 , 160–165) in which it is suggested that three phase transitions occur at ca. 2 GPa, between 8.2 and 9.2 GPa and between 14.0 and 15.5 GPa. In the first two of these transitions the crystal retains its P 2 1 2 1 2 1 symmetry, in the third, although the unit cell dimensions are similar either side of the transition, the space group symmetry drops to P 2 1 . The ambient pressure form is labelled phase I, with the successive high-pressure forms designated I′, II and III, respectively. Phases I and I′ are very similar, the transition being manifested by a slight rotation of the carboxylate group. Phase II, which was found to form between 8.5 and 9.2 GPa, follows the gradual transformation of a long-range electrostatic contact becoming a hydrogen bond between 2.0 and 8.5 GPa, so that the transformation reflects a change in the way the structure accommodates compression rather than a gross change of structure. Phase III, which was found to form above 18.2 GPa in this work, is characterised by the bifurcation of a hydroxyl group in half of the molecules in the unit cell. Density functional theory (DFT) geometry optimisations were used to validate high-pressure structural models and PIXEL crystal lattice and intermolecular interaction energies are used to explain phase stabilities in terms of the intermolecular interactions.
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