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[ÇóÖú] Flapping motion

¸÷λ³æÓÑ£¬Çë½ÌÒ»¸öÎÊÌâÔÚһƪÎÄÏ×£¨J Phys Chem A, 2005, 109, 2078-2089£©Öп´µ½Ò»¾ä»°ÀïµÄÒ»¸ö¶¯×÷²»Ì«Àí½â£¬¹ØÓÚÕâ¸ö¶¯×÷µÄÃèÊöÓÐÕâЩÓï¾ä£º
1. P2083. We have also tried to determine the motion from one saddle structure to the opposite saddled structure (with the other indole rings up and down) through a planar D4h structure (the most commonly adopted by monomeric metallophthalocyanines).

2. P2085. The electronic transitions computed for the D4h conformer are essentially identical in energy, intensity, and character to those computed for the D2d conformer. This indicates that the flapping motion of the molecule from one saddled conformation through the planar "maximum" to the opposite saddled structure, if any, would not be detetable in the optical spectrum.

3. P2088. In solution the theoretical results indicated that it can flap from one D2d-saddled conformation to the opposite one through a D4h-planar structure.

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2. ¶ÔÓÚµÚ¶þ¶ÎÃèÊö£¬ÊÇ·ñÔÚÑо¿flapping motionÊÇ·ñ´æÔÚʱ£¬Ö»Òª¼ÆËã°°Ðνṹ£¨ÕâÀïÊÇD2d£©ºÍÆ½Ãæ½á¹¹£¨D4h£©Á½¸ö¹¹Ð͵路¢Ì¬£¬¿´ËûÃǵ路¢ÄÜ¡¢Ç¿¶ÈºÍÌØÕ÷ÊÇ·ñÒ»Ö£¬Èç¹û˵һÖ£¬ÕâÖÖflapping motion¾Í´æÔÚ£¿
3. µÚÈý¶ÎÊÇ×÷Õߵõ½µÄ½áÂÛ£¬flapping motion´æÔÚ¡£

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