| ²é¿´: 2635 | »Ø¸´: 13 | ||||
| µ±Ç°Ö»ÏÔʾÂú×ãÖ¸¶¨Ìõ¼þµÄ»ØÌû£¬µã»÷ÕâÀï²é¿´±¾»°ÌâµÄËùÓлØÌû | ||||
444239852Òø³æ (ÕýʽдÊÖ)
|
[ÇóÖú]
¹ØÓÚ²¼¾Ö·ÖÎö
|
|||
| ¸÷λ´óÏÀ£¬Ð¡µÜ×î½üÔÚ¼ÆËã¾§ÌåµÄ²¼¾Ö·ÖÎöʱµÃµ½Hirshfeld Charge (e)£¬µ«ÊDz»ÖªµÀHirshfeld Charge (e)ÊÇʲôÒâ˼£¿ÆäÖеÄÕý¸ººÅ´ú±íÊ²Ã´ÄØ£¿ Âé·³¸÷λ£¬Ð¡µÜ²»Ê¤¸Ð¼¤ |
» ²ÂÄãϲ»¶
0703»¯Ñ§Çóµ÷¼Á
ÒѾÓÐ17È˻ظ´
¿¼Ñе÷¼Á-²ÄÁÏÀà-284
ÒѾÓÐ15È˻ظ´
Ò»Ö¾Ô¸211 0703»¯Ñ§ 346·ÖÇóµ÷¼Á
ÒѾÓÐ3È˻ظ´
²ÄÁϹ¤³Ì085601£¬270Çóµ÷¼Á
ÒѾÓÐ24È˻ظ´
085404 293Çóµ÷¼Á
ÒѾÓÐ3È˻ظ´
µ÷¼Á
ÒѾÓÐ21È˻ظ´
¸´ÊÔµ÷¼Á£¬Ò»Ö¾Ô¸Ö£ÖÝ´óѧ²ÄÁÏÓ뻯¹¤289·Ö
ÒѾÓÐ15È˻ظ´
08¹¤¿ÆÇóµ÷¼Á290·Ö
ÒѾÓÐ12È˻ظ´
286Çóµ÷¼Á
ÒѾÓÐ16È˻ظ´
²ÄÁÏÀà284µ÷¼Á
ÒѾÓÐ24È˻ظ´
» ±¾Ö÷ÌâÏà¹Ø¼ÛÖµÌùÍÆ¼ö£¬¶ÔÄúͬÑùÓаïÖú:
baderµçºÉ²¼¾Ö·ÖÎöÔõôÔËÐа¡£¿
ÒѾÓÐ14È˻ظ´
VaspÄܼÆËãµçºÉ×ªÒÆµÄ¾ßÌåÊýֵô£¿
ÒѾÓÐ6È˻ظ´
¹ØÓÚVDDÖÐÔ×ÓµÄWFNÎļþ
ÒѾÓÐ7È˻ظ´
Ôõô¼ÆËãºÍ·ÖÎöµçºÉ×ªÒÆÁ¿
ÒѾÓÐ11È˻ظ´
Mulliken ²¼¾Ö·ÖÎöÈκηÖÎöµçºÉ·Ö²¼¡¢×ªÒƺͻ¯Ñ§ÐÔÖÊ
ÒѾÓÐ10È˻ظ´
²¼¾Ö·ÖÎö ¼ü²¼¾Ö ϵͳ·ÖÎö
ÒѾÓÐ10È˻ظ´
JACSÄÉÃ×½ð°ô×ÏÍâ·ÖÎö
ÒѾÓÐ22È˻ظ´
Çë½Ìbader·ÖÎöÖÐFFT grid (NGXF, NGYF, and NGZF)µÄÉèÖÃ
ÒѾÓÐ24È˻ظ´
²¼¾Ö·ÖÎö²»ÄÜËã~~~ÇóÖú£¡£¡£¡
ÒѾÓÐ11È˻ظ´
[ÇóÖú]¹ØÓÚ̬ÃܶÈͼµÄµ¥Î»ºÍ·ÖÎö
ÒѾÓÐ10È˻ظ´
¡¾ÇóÖú¡¿ÓиßÈË×ö¹ýË®ÄàÊìÁÏÑÒÏà·ÖÎöµÄÂð
ÒѾÓÐ11È˻ظ´
¡¾ÎÄÏ×ѧϰ¡¿JACSÉÏһƪ´¿DFT¼ÆËãµÄÎÄÏ×£º CI-NEB¼ÆË㣬Leuwdin²¼¾Ö·ÖÎö£¬Ì¬ÃܶȷÖÎö
ÒѾÓÐ30È˻ظ´
¡¾ÇóÖú¡¿castep¼ÆËãµçºÉ²¼¾ÖÊý·ÖÎö
ÒѾÓÐ9È˻ظ´
¡¾ÇóÖú¡¿LUMOÒ²¿ÉÒÔÓйìµÀ²¼¾Ö·ÖÎöÂð?
ÒѾÓÐ5È˻ظ´
¡¾ÇóÖú¡¿ÓÃTDDFTÓÅ»¯³öÀ´¼¤·¢Ì¬Ö®ºóµÄ²¼¾Ó·ÖÎö
ÒѾÓÐ20È˻ظ´
¡¾ÇóÖú¡¿²¼¾ÖÊý·ÖÎö
ÒѾÓÐ4È˻ظ´
¡¾ÇóÖú¡¿½ðÊô²ôÔÓ̬ÃܶȷÖÎö
ÒѾÓÐ12È˻ظ´
¡¾ÇóÖú¡¿¹ØÓÚ²¼¾Ö·ÖÎö
ÒѾÓÐ4È˻ظ´
¡¾ÇóÖú¡¿Çó̬ÃܶȼÆËã½á¹û·ÖÎö
ÒѾÓÐ11È˻ظ´
¡¾ÇóÖú¡¿VASPËã²¼¾ÖÊý·ÖÎö
ÒѾÓÐ16È˻ظ´
¡¾ÇóÖú¡¿FukuiÖ¸Êý¼ÆËãÎÊÌ⣿
ÒѾÓÐ10È˻ظ´
444239852
Òø³æ (ÕýʽдÊÖ)
- Ó¦Öú: 20 (СѧÉú)
- ½ð±Ò: 275.9
- É¢½ð: 40
- ºì»¨: 1
- Ìû×Ó: 555
- ÔÚÏß: 268Сʱ
- ³æºÅ: 1146976
- ×¢²á: 2010-11-15
- ÐÔ±ð: GG
- רҵ: Äý¾Û̬ÎïÐÔ II £ºµç×ӽṹ
3Â¥2013-10-08 11:38:06
lq6865387
ľ³æ (ÖøÃûдÊÖ)
ÓÐÖ¾³ÉÄê
- Ó¦Öú: 137 (¸ßÖÐÉú)
- ½ð±Ò: 3328.5
- É¢½ð: 30
- ºì»¨: 18
- Ìû×Ó: 1881
- ÔÚÏß: 150.2Сʱ
- ³æºÅ: 1534707
- ×¢²á: 2011-12-12
- ÐÔ±ð: GG
- רҵ: Äý¾Û̬ÎïÐÔI:½á¹¹¡¢Á¦Ñ§ºÍ

2Â¥2013-10-08 10:57:43
444239852
Òø³æ (ÕýʽдÊÖ)
- Ó¦Öú: 20 (СѧÉú)
- ½ð±Ò: 275.9
- É¢½ð: 40
- ºì»¨: 1
- Ìû×Ó: 555
- ÔÚÏß: 268Сʱ
- ³æºÅ: 1146976
- ×¢²á: 2010-11-15
- ÐÔ±ð: GG
- רҵ: Äý¾Û̬ÎïÐÔ II £ºµç×ӽṹ
4Â¥2013-10-08 17:10:20
pigrass
ר¼Ò¹ËÎÊ (ÖøÃûдÊÖ)
ÒÁ¿¨Ë¹ÌصÄСÖí
-

ר¼Ò¾Ñé: +503 - Ó¦Öú: 377 (˶ʿ)
- ½ð±Ò: 10371
- É¢½ð: 3286
- ºì»¨: 166
- Ìû×Ó: 2101
- ÔÚÏß: 1968.4Сʱ
- ³æºÅ: 1463681
- ×¢²á: 2011-10-27
- ÐÔ±ð: GG
- רҵ: ¸ß·Ö×Ó²ÄÁϽṹÓëÐÔÄÜ
- ¹ÜϽ: ·Ö×ÓÄ£Äâ
¡¾´ð°¸¡¿Ó¦Öú»ØÌû
¡ï ¡ï ¡ï ¡ï ¡ï ¡ï
¸Ðл²ÎÓ룬ӦÖúÖ¸Êý +1
444239852: ½ð±Ò+5, ¡ïÓаïÖú 2013-10-09 21:00:52
sunyang1988: ½ð±Ò+1, лл½»Á÷ 2013-10-11 15:49:25
¸Ðл²ÎÓ룬ӦÖúÖ¸Êý +1
444239852: ½ð±Ò+5, ¡ïÓаïÖú 2013-10-09 21:00:52
sunyang1988: ½ð±Ò+1, лл½»Á÷ 2013-10-11 15:49:25
|
helpÀïµÄ½âÊÍ Hirshfeld charges (Hirshfeld, 1977) are defined relative to the deformation density, this is the difference between the molecular and unrelaxed atomic charge densities. For quantitative descriptions of charge distributions in molecules or solids it is convenient to divide a system into well-defined atomic fragments. A general and natural choice is to share the charge density at each point between the atoms, in proportion to their free-atom densities at the corresponding distances from the nuclei. This prescription yields well-localized bonded-atom distributions each of which closely resembles the molecular density in its vicinity. Integration of the atomic deformation densities - bonded minus free atoms - defines the net atomic charges and multipole moments which concisely summarize the molecular charge reorganization. This permits calculation of the external electrostatic potential and the interaction energy between molecules or between parts of the same molecule. |

5Â¥2013-10-09 16:58:28













»Ø¸´´ËÂ¥
5