TY - JOUR
T1 - 1,4-Bis[2-(4-ferrocenylphenyl)-ethynyl]anthraquinone from synchrotron X-ray powder diffraction
AU - Sachiko, Maki
AU - Nishibori, Eiji
AU - Aoyagi, Shinobu
AU - Sakata, Makoto
AU - Takata, Masaki
AU - Kondo, Mio
AU - Murata, Masaki
AU - Sakamoto, Ryota
AU - Nishihara, Hiroshi
N1 - Copyright:
Copyright 2013 Elsevier B.V., All rights reserved.
PY - 2013/7
Y1 - 2013/7
N2 - The title compound, [Fe2(C5H5) 2(C40H22O2)] or 1,4-(FcPh) 2Aq [where FcPh is 2-(4-ferrocenylphenyl)ethynyl and Aq is anthraquinone], was synthesized in an attempt to obtain a new solvent-incorporating porous material with a large void space. Thermodynamic data for 1,4-(FcPh)2Aq show a phase transition at approximately 430 K. The crystal structure of solvent-free 1,4-(FcPh)2Aq was determined at temperatures of 90, 300 and 500 K using synchrotron powder diffraction data. A direct-space method using a genetic algorithm was employed for structure solution. Charge densities calculated from observed structure factors by the maximum entropy method were employed for model improvement. The final models were obtained through multistage Rietveld refinements. In both phases, the structures of which differ only subtly, the planar Aq fragments are stacked alternately in opposite orientations, forming a one-dimensional column. The FcPh arms lie between the stacks and fill the remaining space, leaving no voids. C - H⋯π interactions between the Ph and Fc fragments mediate crystal packing and stabilization.
AB - The title compound, [Fe2(C5H5) 2(C40H22O2)] or 1,4-(FcPh) 2Aq [where FcPh is 2-(4-ferrocenylphenyl)ethynyl and Aq is anthraquinone], was synthesized in an attempt to obtain a new solvent-incorporating porous material with a large void space. Thermodynamic data for 1,4-(FcPh)2Aq show a phase transition at approximately 430 K. The crystal structure of solvent-free 1,4-(FcPh)2Aq was determined at temperatures of 90, 300 and 500 K using synchrotron powder diffraction data. A direct-space method using a genetic algorithm was employed for structure solution. Charge densities calculated from observed structure factors by the maximum entropy method were employed for model improvement. The final models were obtained through multistage Rietveld refinements. In both phases, the structures of which differ only subtly, the planar Aq fragments are stacked alternately in opposite orientations, forming a one-dimensional column. The FcPh arms lie between the stacks and fill the remaining space, leaving no voids. C - H⋯π interactions between the Ph and Fc fragments mediate crystal packing and stabilization.
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U2 - 10.1107/S0108270113013978
DO - 10.1107/S0108270113013978
M3 - Article
C2 - 23832024
AN - SCOPUS:84880158138
SN - 0108-2701
VL - 69
SP - 696
EP - 703
JO - Acta Crystallographica Section C: Crystal Structure Communications
JF - Acta Crystallographica Section C: Crystal Structure Communications
IS - 7
ER -