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From space group to space groupoid: the partial symmetry of low-temperature E-vanillyl oxime

The phase transition of E-vanillyl oxime {1-[(E)-(hydroxyimino)methyl]-4-hydroxy-3-methoxybenzene, C(8)H(9)NO(3)} has been analysed by single-crystal and powder X-ray diffraction. The high-temperature (HT) phase (P2(1)/a, Z′ = 1) transforms into the low-temperature (LT) phase (threefold superstructu...

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Detalles Bibliográficos
Autores principales: Ehrmann, Katharina, Baudis, Stefan, Stöger, Berthold
Formato: Online Artículo Texto
Lenguaje:English
Publicado: International Union of Crystallography 2019
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6690132/
https://www.ncbi.nlm.nih.gov/pubmed/32830729
http://dx.doi.org/10.1107/S2052520619008461
Descripción
Sumario:The phase transition of E-vanillyl oxime {1-[(E)-(hydroxyimino)methyl]-4-hydroxy-3-methoxybenzene, C(8)H(9)NO(3)} has been analysed by single-crystal and powder X-ray diffraction. The high-temperature (HT) phase (P2(1)/a, Z′ = 1) transforms into the low-temperature (LT) phase (threefold superstructure, [Image: see text], Z′ = 6) at ca 190 K. The point operations lost on cooling, {m ([010]), 2([010])}, are retained as twin operations and constitute the twin law. The screw rotations and glide reflections are retained in the LT phase as partial operations acting on a subset of Euclidean space [Image: see text]. The full symmetry of the LT phase, including partial operations, is described by a disconnected space groupoid which is built of three connected components.