| ²é¿´: 371 | »Ø¸´: 2 | ||
| µ±Ç°Ö»ÏÔʾÂú×ãÖ¸¶¨Ìõ¼þµÄ»ØÌû£¬µã»÷ÕâÀï²é¿´±¾»°ÌâµÄËùÓлØÌû | ||
oneil½ð³æ (ÕýʽдÊÖ)
|
[ÇóÖú]
¸ß˹¼¤·¢Ì¬ÓÅ»¯¹ØÓÚÎÄÏ×ÃèÊö×÷ÒµÉèÖÃÇë½Ì
|
|
|
¸÷룬ÎÒ×î½üÔÚÁ·Ï°gaussian¼¤·¢Ì¬µÄÓÅ»¯£¬ÓÐһƪÎÄÏ×Ìáµ½ÕâÑùÒ»¶Î»°£ºThe absorption spectra have been calculated by the Time Depedent PBE0/6-311+G(2d,2p) calculations performed on geometries optimized at the PBE0 6-31+G(d,p) level. Numerical excited state geometry optimizations have been performed at the the TD/PBE0 6-31G(d) level, without any planarity constraint. All the gradients are smaller than 0.02 eV/bohr for the excited state geometry optimizations performed in vacuo and smaller than 0.05 eV/bohr for the geometry optimizations performed in aqueous solution and Hydrogen atom degrees of freedom are frozen at their value optimized in the gas phase. ÎÒÏëÎÊÏ£¬Õâ¸ö0.02ev/bohrËûÊÇÔõô×öµ½µÄ£¬gaussian×÷Òµ¹Ø¼ü×ÖÔõôд£¬³õѧÁ¿»¯£¬ÇëÖ¸½Ì£¬ÏÈллÁË£¡ |
» ²ÂÄãϲ»¶
2026ºþ±±Ê¦·¶´óѧ»¯Ñ§»¯¹¤Ñ§ÔºÕÐÊÕÑо¿Éúµ÷¼Á
ÒѾÓÐ0È˻ظ´
26Äê²ÄÁÏ/»¯Ñ§Ïà¹Ø×¨Òµ²©Ê¿Ñо¿ÉúÕÐÉú ÎÂÖÝ´óѧ»¯Ñ§Óë²ÄÁϹ¤³ÌѧԺ(26ÄêÇï¼¾Èëѧ)
ÒѾÓÐ0È˻ظ´
ÎïÀí»¯Ñ§ÂÛÎÄÈóÉ«/·ÒëÔõôÊÕ·Ñ?
ÒѾÓÐ58È˻ظ´
0703µ÷¼Á
ÒѾÓÐ2È˻ظ´
2026Ä격ʿÑо¿ÉúÕÐÉú
ÒѾÓÐ1È˻ظ´
304Çóµ÷¼Á
ÒѾÓÐ6È˻ظ´
Ò»Ö¾Ô¸ÄÏʦ´ó0703»¯Ñ§ 275Çóµ÷¼Á
ÒѾÓÐ4È˻ظ´
A Çø¹ýÏ߾ͿÉÉê£¡ÖØÇìË«·Ç¹«°ì¸ßУ 0856µ÷¼Á£¬½ÓÊÜ¿çרҵ£¡ÄÉÃײÄÁÏ / Èó»¬ÈÈÃÅ·½Ïò
ÒѾÓÐ0È˻ظ´
¹ØÓÚÑо¿Éúµ÷¼ÁµÄЩÐí½¨Òé
ÒѾÓÐ1È˻ظ´
Çóµç×ÓÊé¡¶»·ºý¾«»¯Ñ§ : »ù´¡ÓëÓ¦Óá·
ÒѾÓÐ0È˻ظ´
oneil
½ð³æ (ÕýʽдÊÖ)
- Ó¦Öú: 2 (Ó×¶ùÔ°)
- ½ð±Ò: 1353
- É¢½ð: 101
- Ìû×Ó: 358
- ÔÚÏß: 78.8Сʱ
- ³æºÅ: 1108782
- ×¢²á: 2010-09-27
- ÐÔ±ð: GG
- רҵ: ¹âѧºÍ¹âµç×Ó²ÄÁÏ
3Â¥2012-11-17 23:43:05
shuangliu
гæ (СÓÐÃûÆø)
- Ó¦Öú: 14 (СѧÉú)
- ½ð±Ò: 625.7
- É¢½ð: 20
- Ìû×Ó: 162
- ÔÚÏß: 48.7Сʱ
- ³æºÅ: 1409543
- ×¢²á: 2011-09-20
- רҵ: ÀíÂۺͼÆË㻯ѧ
2Â¥2012-11-17 16:59:09














»Ø¸´´ËÂ¥