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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«ÊDzéÁËÔʼµÄÎÄÏ×£¬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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aylayl08(½ð±Ò+1):лл 2010-06-09 16:31:08
aylayl08(½ð±Ò+1):лл 2010-06-09 16:31:08
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3Â¥2010-06-08 08:01:22
Miracle922
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aylayl08(½ð±Ò+2):ллÌáʾ 2010-06-09 16:31:51
aylayl08(½ð±Ò+2):ллÌáʾ 2010-06-09 16:31:51
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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 |

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