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Miracle922

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[½»Á÷] ¡¾ÌÖÂÛ¡¿ÉîÎÊ£ºÔ­×Ó¹ìµÀ¶Ô·Ö×Ó¹ìµÀµÄ¹±Ï×£¬º¯ÊýÈçºÎÈçºÎ¹éÊôµ½Ô­×Ó¹ìµÀÀ

ÔÚ6-311+G(d)»ù×éÏ£¬ÓÃpop=fullµÃµ½molecular orbital coefficients£¬ÈçÏÂËùʾ£º


1  Al  1S        
2        2S      
3        3S      
4        4S      
5        5S      
6        6S      
7        7PX   
8        7PY   
9        7PZ     
10        8PX   
11        8PY   
12        8PZ   
13        9PX   
14        9PY   
15        9PZ   
16       10PX  
17       10PY  
18       10PZ   
19       11PX  
20       11PY  
21       11PZ   
22       12S     
23       12PX  
24       12PY  
25       12PZ   
26       13D 0  
27       13D+1
28       13D-1
29       13D+2
30       13D-2

91    Ti  1S  
92        2S   
93        3S     
94        4S     
95        5S     
96        6S     
97        7S     
98        8S     
99        9S      
100       10PX  
101       10PY  
102       10PZ  
103       11PX  
104       11PY  
105       11PZ  
106       12PX  
107       12PY  
108       12PZ  
109       13PX  
110       13PY  
111       13PZ  
112       14PX  
113       14PY  
114       14PZ  
115       15D 0
116       15D+1
117       15D-1
118       15D+2
119       15D-2
120       16D 0
121       16D+1
122       16D-1
123       16D+2
124       16D-2
125       17D 0
126       17D+1
127       17D-1
128       17D+2
129       17D-2
130       18S     
131       19PX  
132       19PY  
133       19PZ  
134       20PX  
135       20PY  
136       20PZ  
137       21D 0
138       21D+1
139       21D-1
140       21D+2
141       21D-2
142       22F 0  
143       22F+1
144       22F-1
145       22F+2
146       22F-2
147       22F+3
148       22F-3

ÕâЩ(s pd f)º¯ÊýÓ¦¸ÃÊǶÔÓ¦ÓÚAl£¨»òTi)µÄijһԺ×Ó¹ìµÀ£¬±ÈÈç˵2s,3p,3dÖ®ÀàµÄ£¬µ«ÊDzéÁËԭʼµÄÎÄÏ×£¬Ò²¿ÉÄÜÊÇûÓÐÍêÈ«Ã÷°×£¬×îÖÕû·¨µÃµ½È·ÇеĹéÊô£¬Ò²¾ÍÊÇ˵ µÚ¶þÁÐÓ¦¸ÃÍêÈ«¿ÉÒÔ¹éÊôµ½¾ßÌåµÄÔ­×Ó¹ìµÀ£¬±ÈÈç˵ÉÏÃæÄ³Ò»ÐжÔÓ¦ÄĸöÔ­×ÓµÄÄĸö¹ìµÀ¡£Õâ¸ö¹éÊôÆðÀ´Ê×ÏÈÊÇҪȷ¶¨»ù×麬Ò壬¿ÉÄÜÉæ¼°µ½ºÜ¶àÄÚÈݸö£¬²»ÖªµÀÄÄλ¶ÔÕâ·½ÃæÊìϤ£¬¿ÉÒÔÌÖÂÛÏ£»Èç¹ûÓÐ×öÕâ¿é¹éÊôµÄͬÐÐÌÖÂÛÄǸüºÃÁË£¬ºÜÏëŪÃ÷°×Õâ¸öÎÊÌâ¡£ÎÒÒÔǰҲ¿´µ½¹ýһλ°æÖ÷¸ø³öÁËÏà¹ØµÄÎÄÏ×£¬µ«ÊÇ»¹ÊÇÄÑÒÔÞÛ˳£¬¶Ô6-311+G(d)Õâ¸ö»ù×é»òÀàËÆµÄ»ù×黹²»ÊǺÜÃ÷°×£¬ÈçÓÐÄÄλ³æÓѶԴ˸ÐÐËȤ£¬¿ÉÒÔÒ»ÆðÌÖÂÛ




+++++++++++++++++++++++++++++++++++++++++++++++++

ÒÔÏÂÊÇGaussian ¼¼ÊõÖ§³ÖµÄ»Ø¸´£¬Ï£Íû¶Ô¸ÐÐËȤµÄ³æÓÑÓÐËù°ïÖú¡£

Dr. Xu,
      Thank you for giving us a chance to comment.
      The first and probably least satisfying answer is that you really
cannot make a correspondence between the basis functions used in this
calculation and the atomic orbitals of a QM description of an atom.  The
basis set is a mathematical construction which is much less flexible
than the real orbitals and thus many more functions are included in an
attempt to span the space and linear combinations of these functions,
LCAOs, become the MO functions which solve the SCF equations.  The numbers
on these functions (1S,2S,...7Px,...) have no relation to quantum numbers
but rather enumerate the functions on a given atom, 1-N functions.
      The second answer is that the 6-311++G(d) basis set is constructed
with core type functions formed from fixed linear combinations of simple
or primitive gaussians and in the case of Si the first 2 functions are
intended to reproduce 1S and 2S and the first p functions are 2P(x,y,z).
Then the valence 3S and 3P atomic orbitals are represented by 3s and 4s
from the basis set and 2p(x,y,z) and 3p(x,y,z) where I have used lower
case for basis functions and upper case for atomic orbitals.  The additional
s and p functions contribute to a lesser degree to all of the MOs and
the d functions are polarization functions which only contribute to the
occupied MOs indirectly, mixing in with AO functions on other atoms.  A
similar analysis can be applied to V but neither of these is a one to one
correspondence with the atomic orbitals, nor is it intended as such.
      Perhaps a more useful answer in terms of numerical values is to use
the Pop=Orbitals analysis and look in the Mulliken analysis.  It gives a
breakdown of each MO in terms of s, p, d contributions from various atoms.
You don't get a correspondence with atomic orbitals but you do get the
weight of each atom in a given MO.
      Does this help?
On Mon, Jun 07, 2010 at 10:51:40AM -0400

[ Last edited by Miracle922 on 2010-6-8 at 10:36 ]
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fooo

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¡ï
aylayl08(½ð±Ò+1):лл 2010-06-09 16:31:08
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ÒýÓûØÌû:
Originally posted by Miracle922 at 2010-06-07 23:54:37:
ÔÚ6-311+G(d)»ù×éÏ£¬ÓÃpop=fullµÃµ½molecular orbital coefficients£¬ÈçÏÂËùʾ£º


1  Al  1S        
2        2S      
3        3S      
4        4S      
5        5S      
6        6S      ...

2Â¥2010-06-08 03:12:26
ÒÑÔÄ   »Ø¸´´ËÂ¥   ¹Ø×¢TA ¸øTA·¢ÏûÏ¢ ËÍTAºì»¨ TAµÄ»ØÌû

quantumor

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3Â¥2010-06-08 08:01:22
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Miracle922

Í­³æ (ÕýʽдÊÖ)

¡ï ¡ï
aylayl08(½ð±Ò+2):ллÌáʾ 2010-06-09 16:31:51
ÒÔÏÂÊÇGaussian ¼¼ÊõÖ§³ÖµÄ»Ø¸´£¬Ï£Íû¶Ô¸ÐÐËȤµÄ³æÓÑÓÐËù°ïÖú¡£

Dr. Xu,
      Thank you for giving us a chance to comment.
      The first and probably least satisfying answer is that you really
cannot make a correspondence between the basis functions used in this
calculation and the atomic orbitals of a QM description of an atom.  The
basis set is a mathematical construction which is much less flexible
than the real orbitals and thus many more functions are included in an
attempt to span the space and linear combinations of these functions,
LCAOs, become the MO functions which solve the SCF equations.  The numbers
on these functions (1S,2S,...7Px,...) have no relation to quantum numbers
but rather enumerate the functions on a given atom, 1-N functions.
      The second answer is that the 6-311++G(d) basis set is constructed
with core type functions formed from fixed linear combinations of simple
or primitive gaussians and in the case of Si the first 2 functions are
intended to reproduce 1S and 2S and the first p functions are 2P(x,y,z).
Then the valence 3S and 3P atomic orbitals are represented by 3s and 4s
from the basis set and 2p(x,y,z) and 3p(x,y,z) where I have used lower
case for basis functions and upper case for atomic orbitals.  The additional
s and p functions contribute to a lesser degree to all of the MOs and
the d functions are polarization functions which only contribute to the
occupied MOs indirectly, mixing in with AO functions on other atoms.  A
similar analysis can be applied to V but neither of these is a one to one
correspondence with the atomic orbitals, nor is it intended as such.
      Perhaps a more useful answer in terms of numerical values is to use
the Pop=Orbitals analysis and look in the Mulliken analysis.  It gives a
breakdown of each MO in terms of s, p, d contributions from various atoms.
You don't get a correspondence with atomic orbitals but you do get the
weight of each atom in a given MO.
      Does this help?
On Mon, Jun 07, 2010 at 10:51:40AM -0400
×öµ½¼«Ö£¬×öµ½Ï¸´¦
4Â¥2010-06-08 10:36:08
ÒÑÔÄ   »Ø¸´´ËÂ¥   ¹Ø×¢TA ¸øTA·¢ÏûÏ¢ ËÍTAºì»¨ TAµÄ»ØÌû
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