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Single-crystal structure analysis of non-deuterated triglycine sulfate by neutron diffraction at 20 and 298 K: a new disorder model for the 298 K structure

Precise single-crystal structure analyses of the title compound, bis­(glycinium) sulfate–glycine (1/1), 2C(2)H(6)NO(2) (+)·SO(4) (2−)·C(2)H(5)NO(2) (or C(6)H(17)N(3)O(10)S), non-deuterated triglycine sulfate (HTGS) at 20 K and 298 K were undertaken using time-of-flight neutron diffraction data. At 2...

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Detalles Bibliográficos
Autores principales: Terasawa, Yukana, Ohhara, Takashi, Sato, Sota, Yoshida, Satoshi, Asahi, Toru
Formato: Online Artículo Texto
Lenguaje:English
Publicado: International Union of Crystallography 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8900510/
https://www.ncbi.nlm.nih.gov/pubmed/35371538
http://dx.doi.org/10.1107/S2056989022000858
Descripción
Sumario:Precise single-crystal structure analyses of the title compound, bis­(glycinium) sulfate–glycine (1/1), 2C(2)H(6)NO(2) (+)·SO(4) (2−)·C(2)H(5)NO(2) (or C(6)H(17)N(3)O(10)S), non-deuterated triglycine sulfate (HTGS) at 20 K and 298 K were undertaken using time-of-flight neutron diffraction data. At 20 K for the O—H⋯O hydrogen bond between the glycinium cation and the zwitterionic, unprotonated glycine mol­ecule that is associated with the ferroelectric behaviour of HTGS, O—H = 1.070 (3), H⋯O = 1.408 (3) [δ = 0.338 (4)], O⋯O = 2.4777 (15) Å and O—H⋯O = 179.0 (4)°, which is in good agreement with previous studies. Two reasonable structures for the same three atoms were refined for the 298 K dataset. One is a single-minimum potential-energy model, with O—H = 1.090 (12), H⋯O = 1.361 (12) [δ = 0.271 (17)], O⋯O = 2.450 (7) Å and O—H⋯O = 179.2 (10)°, having the H atom with a large ellipticity along the bond path between the O atoms. The other is a double-minimum potential-energy model having two H atom sites with occupancies of 0.876 (8) and 0.124 (8): for the major occupancy component, O—H = 1.065 (12), H⋯O = 1.387 (12), O⋯O = 2.451 (7) Å and O—H⋯O = 178.2 (11)° and for the minor component, O—H = 1.06 (4), H⋯O = 1.41 (4), O⋯O = 2.451 (7) Å and O—H⋯O = 166 (2)°. These models did not show any significant differences in R factors. In addition, the unit-cell parameters and other structural parameters of HTGS did not show any major differences compared to those of partially deuterated TGS and fully deuterated TGS for both 20 K and 298 K.