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On the basis of the structure data of single-crystal diffraction, the packing geometries of TPA-CO at 0.0 GPa, 1.0 GPa and 2.0 GPa along the c axis were optimized by DFT calculations. The optimized structure at 0.0 GPa was in agreement with that of single crystals (see Table S1 and S2† . Notably, the dihedral angle (q1, q2) between the carbonyl group and the neighbouring benzene ring was smaller at 2.0 GPa than at 0 GPa, as shown in Table S2.† Clearly, pressurization reduced the void volumes and densified the molecular packing, which induced the structural planarization. Single crystals of TPA-CO were obtained by slow evaporation of n-hexane¨CCH2Cl2. As depicted in Fig. S8B and S9C,† the aromatic C¨CH¡¤¡¤¡¤¦Ð and multiple C¨CH¡¤¡¤¡¤O interactions made the adjacent twisted molecules connect together and form ¡°molecular sheets¡±. Another C¨CH¡¤¡¤¡¤O interaction with a distance of 2.8616 A ˚ was also observed between the neighbouring sheets (Fig. S8B† . Usually, for D¨Cp¨CA dipolemolecules, the dipole interaction places the ¡°A¡±group of one molecule above the ¡°D¡± moiety of its neighbouring molecule, which contributes to the stability of the crystalline state.In this case, the A (D) moiety of one molecule was placed above the A (D) moiety of another adjacent molecule, as shown in Fig. 5. As a result, the D¨Cp¨CA dipole¨Cdipole interactions were mutually repulsive, which implied that these neighbouring molecules could not be clustered closely together even under external stimuli. |
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ÍÅ×ÓС½ã: ½ð±Ò+11, ·ÒëEPI+1, ¡ï¡ï¡ï¡ï¡ï×î¼Ñ´ð°¸, лл 2014-10-16 11:51:27
ÍÅ×ÓС½ã: ½ð±Ò+11, ·ÒëEPI+1, ¡ï¡ï¡ï¡ï¡ï×î¼Ñ´ð°¸, лл 2014-10-16 11:51:27
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. Notably, the dihedral angle (q1, q2) between the carbonyl group and the neighbouring benzene ring was smaller at 2.0 GPa than at 0 GPa, as shown in Table S2.† Clearly, pressurization reduced the void volumes and densified the molecular packing, which induced the structural planarization. Single crystals of TPA-CO were obtained by slow evaporation of n-hexane¨CCH2Cl2. As depicted in Fig. S8B and S9C,† the aromatic C¨CH¡¤¡¤¡¤¦Ð and multiple C¨CH¡¤¡¤¡¤O interactions made the adjacent twisted molecules connect together and form ¡°molecular sheets¡±. Another C¨CH¡¤¡¤¡¤O interaction with a distance of 2.8616 A ˚ was also observed between the neighbouring sheets (Fig. S8B†
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