TY - JOUR
T1 - Role of Steric Hindrance in the Crystal Packing of Z′ = 4 Superstructure of Trimethyltin Hydroxide
AU - Dey, S.
AU - Schönleber, A.
AU - Mondal, S.
AU - Ali, S. I.
AU - van Smaalen, S.
N1 - KAUST Repository Item: Exported on 2020-10-01
Acknowledgements: The authors thank Carsten Paulmann for assistance in the diffraction experiments at beamline F1 of Hasylab at DESY, Hamburg. The authors thank Karen Friese and Vaclav Petricek for useful discussions. Financial support has been obtained from the German Science Foundation (DFG) under grant number SCHO 830/3-1.
PY - 2018/1/22
Y1 - 2018/1/22
N2 - The roomerature crystal structure of trimethyltin hydroxide, (CH)SnOH, has been described by Anderson et al. [Cryst. Growth Des. 2011, 11, 820-826] as a 2a × 2b × 8c, 32-fold superstructure. We report a a × b × 8c, eight-fold superstructure with orthorhombic P2cn symmetry and Z′ = 4. Structured diffuse scattering observed at the positions of presumed superlattice reflections along a∗ and b∗ might have appeared as Bragg reflections in the experiment by Anderson et al. Alternatively, Anderson et al. and the present work might have studied different polymorphs of (CH)SnOH. Crystalline (CH)SnOH constitutes polymeric chains arranged parallel to c. In the eight-fold superstructure at 220 K, the polymeric chains possess a distorted zigzag arrangement of linked linear O-Sn-O units with bent angle at oxygen of ∼139.2°. This structure is essentially different from the 8-helical arrangement in the published 32-fold superstructure model. The origin of the distorted zigzag structure is explained by steric hindrance between hydrogen atoms of adjacent hydroxy groups and (CH)Sn groups. Frustration in the packing of the chains is determined by steric hindrance between methyl groups of neighboring chains, which prevents the formation of interchain C-H···O hydrogen bonds.
AB - The roomerature crystal structure of trimethyltin hydroxide, (CH)SnOH, has been described by Anderson et al. [Cryst. Growth Des. 2011, 11, 820-826] as a 2a × 2b × 8c, 32-fold superstructure. We report a a × b × 8c, eight-fold superstructure with orthorhombic P2cn symmetry and Z′ = 4. Structured diffuse scattering observed at the positions of presumed superlattice reflections along a∗ and b∗ might have appeared as Bragg reflections in the experiment by Anderson et al. Alternatively, Anderson et al. and the present work might have studied different polymorphs of (CH)SnOH. Crystalline (CH)SnOH constitutes polymeric chains arranged parallel to c. In the eight-fold superstructure at 220 K, the polymeric chains possess a distorted zigzag arrangement of linked linear O-Sn-O units with bent angle at oxygen of ∼139.2°. This structure is essentially different from the 8-helical arrangement in the published 32-fold superstructure model. The origin of the distorted zigzag structure is explained by steric hindrance between hydrogen atoms of adjacent hydroxy groups and (CH)Sn groups. Frustration in the packing of the chains is determined by steric hindrance between methyl groups of neighboring chains, which prevents the formation of interchain C-H···O hydrogen bonds.
UR - http://hdl.handle.net/10754/627466
UR - https://pubs.acs.org/doi/10.1021/acs.cgd.7b01295
UR - http://www.scopus.com/inward/record.url?scp=85043292159&partnerID=8YFLogxK
U2 - 10.1021/acs.cgd.7b01295
DO - 10.1021/acs.cgd.7b01295
M3 - Article
SN - 1528-7483
VL - 18
SP - 1394
EP - 1400
JO - Crystal Growth & Design
JF - Crystal Growth & Design
IS - 3
ER -