Data for the configuration selection module is initiated with the SELECT directive, followed by those directives characterising the symmetry of the state(s) of interest and reference configurations (CNTRL, SPIN, SYMMETRY, CONF etc.) and terminated by data (ROOTS, THRESH) controlling the process of selection.
Example
SPIN 3
SPIN TRIPLET
are equivalent; the wavefunction will be three-fold spin degenerate.
Example
In a system of C2v symmetry, the data line
SYMMETRY 3
would be required when performing calculations on states of
B2 symmetry. Failure to present the directive in such
cases will lead to the default A1 symmetry.
Example
Presenting the data line
SINGLES 1
in a Table-CI calculation of a closed-shell system, where the
SCF configuration is the first in the CONF list, will lead
to the inclusion of all single excitations with respect to the
SCF function in the final CI. Such inclusion leads, of course, to
a marked improvement in the quality of one-electron properties
computed from the CI wavefunction.
| Orbital | IRrep | |
|
C
|
C2v | Sequence No. |
|
a1 | 1 |
|
|
||
| b1 | 2 | |
| b2 | 3 | |
|
|
a2 | 4 |
| Orbital | IRrep | |
|
D
|
D2h | Sequence No. |
|
ag | 1 |
|
|
||
| b3u | 2 | |
| b2u | 3 | |
|
|
b1g | 4 |
|
|
b1u | 5 |
|
|
||
| b2g | 6 | |
| b3g | 7 | |
|
|
au | 8 |
Example 1
Consider performing a valence-CI calculation on the PH3 molecule using a 6-31G(*) basis. While the molecular symmetry is C3v, the symmetry adaptation and subsequent CI will be conducted in the Cs point group. An examination of the SCF output reveals the following orbital analysis.
=============================
IRREP NO. OF SYMMETRY ADAPTED
BASIS FUNCTIONS
=============================
1 18
2 7
=============================
and the following orbital assignments characterising the closed-shell
SCF configuration:
| 1a122a121e43a124a122e45a12 | (1) |
| 1a'22a'21a''23a'24a'25a'26a'22a''27a'2 | (2) |
===============================================
M.O. IRREP ORBITAL ENERGY ORBITAL OCCUPANCY
===============================================
1 1 -79.93661395 2.0000000
2 1 -7.48916431 2.0000000
3 1 -5.38319410 2.0000000
4 2 -5.38319405 2.0000000
5 1 -5.38149104 2.0000000
6 1 -0.85610769 2.0000000
7 1 -0.52191424 2.0000000
8 2 -0.52191424 2.0000000
9 1 -0.38579686 2.0000000
10 1 0.16819544 0.0000000
11 2 0.16819544 0.0000000
12 1 0.26587776 0.0000000
13 1 0.46072690 0.0000000
14 2 0.46072690 0.0000000
15 1 0.47871033 0.0000000
16 1 0.56106989 0.0000000
17 1 0.89229884 0.0000000
18 2 0.89229885 0.0000000
19 2 0.91131383 0.0000000
20 1 0.91131383 0.0000000
21 1 0.93118300 0.0000000
22 1 1.17900613 0.0000000
23 2 1.45058658 0.0000000
24 1 1.45058658 0.0000000
25 1 3.78674557 0.0000000
===============================================
Based on the above output, the CONF data lines may be
deduced from the following table, where we
assume that we wish to freeze the five inner shell orbitals:
| 1a'22a'21a''23a'24a'2 | (3) |
| IRrep | IRrep | No. of Basis | Frozen | Active | Sequence |
| No. | Functions | MOs | MOs | Nos. | |
| a' | 1 | 18 | 4 | 14 | 1-14 |
| a'' | 2 | 7 | 1 | 6 | 15-20 |
| 5a'28a'22a''27a'2 | (4) |
| 5a'26a'23a''27a'2 | (5) |
CONF
0 1 2 3 15
0 1 3 4 15
0 1 2 3 16
The complete data file for performing the
SCF and subsequent CI would then be as follows:
TITLE
PH3 * 6-31G* VALENCE-CI 3M/1R
SUPER OFF NOSYM
ZMAT
P
H 1 RPH
H 1 RPH 2 THETA
H 1 RPH 2 THETA 3 THETA 1
VARIABLES
RPH 2.685
THETA 93.83
END
BASIS 6-31G*
RUNTYPE CI
MRDCI
TRAN CORE
4 1
1 TO 4 1
SELECT
SINGLES 1
CONF
0 1 2 3 15
0 1 3 4 15
0 1 2 3 16
NATORB
ENTER
Example 2
In this example we wish to perform a valence-CI calculation on the CuCl molecule using a 3-21G basis. While the molecular symmetry is C
v,
the symmetry adaptation and subsequent CI will be conducted in the
C2v point group. The resolution of the C
v into the C2v orbital species is given in Table 2. An examination of the
SCF output reveals the following orbital analysis.
=============================
IRREP NO. OF SYMMETRY ADAPTED
BASIS FUNCTIONS
=============================
1 22
2 9
3 9
4 2
=============================
and the following orbital assignments from the converged closed shell SCF:
===============================================
M.O. IRREP ORBITAL ENERGY ORBITAL OCCUPANCY
===============================================
1 1 -326.84723972 2.0000000
2 1 -104.02836336 2.0000000
3 1 -40.71695637 2.0000000
4 1 -35.46377378 2.0000000
5 3 -35.45608069 2.0000000
6 2 -35.45608068 2.0000000
7 1 -10.42193940 2.0000000
8 1 -7.88512031 2.0000000
9 2 -7.88222844 2.0000000
10 3 -7.88222844 2.0000000
11 1 -5.07729175 2.0000000
12 1 -3.38247056 2.0000000
13 3 -3.35978308 2.0000000
14 2 -3.35978307 2.0000000
15 1 -1.01099628 2.0000000
16 3 -0.53702948 2.0000000
17 2 -0.53702947 2.0000000
18 4 -0.49640067 2.0000000
19 1 -0.49640067 2.0000000
20 1 -0.44715317 2.0000000
21 3 -0.39988537 2.0000000
22 2 -0.39988537 2.0000000
23 1 -0.35127248 2.0000000
24 1 0.00023285 0.0000000
25 3 0.06300102 0.0000000
26 2 0.06300102 0.0000000
27 1 0.12855448 0.0000000
28 1 0.19287013 0.0000000
29 3 0.25729975 0.0000000
30 2 0.25729975 0.0000000
31 1 0.39720201 0.0000000
32 1 0.86197727 0.0000000
33 2 0.88942618 0.0000000
34 3 0.88942618 0.0000000
35 1 1.01877167 0.0000000
36 1 2.16694989 0.0000000
37 3 3.96181512 0.0000000
38 2 3.96181512 0.0000000
39 4 3.98212497 0.0000000
40 1 3.98212497 0.0000000
41 1 4.08851360 0.0000000
42 1 24.51368240 0.0000000
===============================================
Based on the above output, the CONF data lines may be
deduced from the following table, where we
assume that we wish to freeze the first 14 inner shell orbitals:
|
1 |
(6) |
| IRrep | IRrep | No. of Basis | Frozen | Active | Sequence |
| No. | Functions | MOs | MOs | Nos. | |
| a1 | 1 | 22 | 8 | 14 | 1-14 |
| b1 | 2 | 9 | 3 | 6 | 15-20 |
| b2 | 3 | 9 | 3 | 6 | 21-26 |
| a2 | 4 | 2 | 0 | 2 | 27-28 |
|
9 |
(7) |
CONF
0 1 2 3 4 15 16 21 22 27
The complete data file for performing the
SCF and subsequent CI would then be as follows:
TITLE\CUCL .. 3-21G
ZMAT ANGSTROM\CU\CL 1 CUCL\
VARIABLES\CUCL 2.093 \END
BASIS 3-21G
RUNTYPE CI
MRDCI
TRAN CORE
8 3 3 0
1 TO 8 1 TO 3 1 TO 3
SELECT
SINGLES 1
CONF
0 1 2 3 4 15 16 21 22 27
NATORB
ENTER
The inclusion of a second reference configuration corresponding to
the doubly excited configuration
|
9 |
(8) |
CONF
0 1 2 3 4 15 16 21 22 27
0 1 2 3 5 15 16 21 22 27
Example 3
Consider performing a valence-CI calculation on the SiH4 molecule using a 6-31G(*) basis. While the molecular symmetry is Td, the symmetry adaptation and subsequent CI will be conducted in the C2v point group. An examination of the SCF output reveals the following orbital analysis.
=============================
IRREP NO. OF SYMMETRY ADAPTED
BASIS FUNCTIONS
=============================
1 9
2 6
3 6
4 6
=============================
and the following orbital assignments from
the converged closed shell SCF:
===============================================
M.O. IRREP ORBITAL ENERGY ORBITAL OCCUPANCY
===============================================
1 1 -68.77130710 2.0000000
2 1 -6.12943325 2.0000000
3 2 -4.23503117 2.0000000
4 3 -4.23503117 2.0000000
5 4 -4.23503117 2.0000000
6 1 -0.73046864 2.0000000
7 4 -0.48480821 2.0000000
8 3 -0.48480821 2.0000000
9 2 -0.48480821 2.0000000
10 2 0.16291387 0.0000000
11 3 0.16291387 0.0000000
12 4 0.16291387 0.0000000
13 1 0.25681257 0.0000000
14 1 0.33606346 0.0000000
15 3 0.37087856 0.0000000
16 2 0.37087856 0.0000000
17 4 0.37087856 0.0000000
18 1 0.79946861 0.0000000
19 1 0.79946861 0.0000000
20 4 0.86232544 0.0000000
21 3 0.86232544 0.0000000
22 2 0.86232544 0.0000000
23 1 1.23833149 0.0000000
24 4 1.44033091 0.0000000
25 3 1.44033091 0.0000000
26 2 1.44033091 0.0000000
27 1 3.13181655 0.0000000
===============================================
Based on the above output, the CONF data lines may be
deduced from the following table, where we
assume that we wish to freeze the first 5 silicon inner shell orbitals:
| IRrep | IRrep | No. of Basis | Frozen | Active | Sequence |
| No. | Functions | MOs | MOs | Nos. | |
| a1 | 1 | 9 | 2 | 7 | 1-7 |
| b1 | 2 | 6 | 1 | 5 | 8-12 |
| b2 | 3 | 6 | 1 | 5 | 13-17 |
| a2 | 4 | 6 | 1 | 5 | 18-22 |
CONF
0 1 8 13 18
The complete data file for performing the
SCF and subsequent CI would then be as follows:
TITLE
SIH4 * 6-31G* MRDCI VALENCE-CI 1M/1R
ZMAT
SI
H 1 SIH
H 1 SIH 2 109.471
H 1 SIH 2 109.471 3 120.0
H 1 SIH 2 109.471 4 120.0
VARIABLES
SIH 2.80
END
BASIS 6-31G*
RUNTYPE CI
MRDCI
TRAN CORE
2 1 1 1
1 2 1 1 1
SELECT
CONF
0 1 8 13 18
SINGLES 1
NATORB
ENTER
Example 4
In this example we wish to perform a valence-CI calculation on the
N2 molecule using a 4-31G(*) basis. While the molecular symmetry is
D
h, the symmetry adaptation and subsequent CI will be conducted in
the D2h point group. The resolution of the D
h into the D2h orbital species is given in Table 2. An examination of the
SCF output reveals the following orbital analysis.
=============================
IRREP NO. OF SYMMETRY ADAPTED
BASIS FUNCTIONS
=============================
1 8
2 3
3 3
4 1
5 8
6 3
7 3
8 1
=============================
and the following orbital assignments from the converged closed shell SCF:
===============================================
M.O. IRREP ORBITAL ENERGY ORBITAL OCCUPANCY
===============================================
1 1 -15.65951533 2.0000000
2 5 -15.65474750 2.0000000
3 1 -1.50615941 2.0000000
4 5 -0.75782277 2.0000000
5 1 -0.63244925 2.0000000
6 3 -0.63135826 2.0000000
7 2 -0.63135826 2.0000000
8 6 0.20154861 0.0000000
9 7 0.20154861 0.0000000
10 5 0.63883097 0.0000000
11 1 0.82491489 0.0000000
12 3 0.89634343 0.0000000
13 2 0.89634343 0.0000000
14 1 0.91812387 0.0000000
15 7 1.10036132 0.0000000
16 6 1.10036132 0.0000000
17 5 1.17625689 0.0000000
18 5 1.66995008 0.0000000
19 4 1.70518236 0.0000000
20 1 1.70518236 0.0000000
21 3 1.91001614 0.0000000
22 2 1.91001614 0.0000000
23 8 2.29436539 0.0000000
24 5 2.29436539 0.0000000
25 1 2.84356916 0.0000000
26 7 3.00847817 0.0000000
27 6 3.00847817 0.0000000
28 5 3.37447679 0.0000000
29 1 3.71753400 0.0000000
30 5 4.09917273 0.0000000
===============================================
Based on the above output, the CONF data lines may be
deduced from the following table, where we
assume that we wish to freeze the two N1s inner shell orbitals:
| IRrep | IRrep | No. of Basis | Frozen | Active | Sequence |
| No. | Functions | MOs | MOs | Nos. | |
|
|
1 | 8 | 1 | 7 | 1-7 |
| 2 | 3 | 0 | 3 | 8-10 | |
| 3 | 3 | 0 | 3 | 11-13 | |
|
|
4 | 1 | 0 | 1 | 14 |
|
|
5 | 8 | 1 | 7 | 15-21 |
| 6 | 3 | 0 | 3 | 22-24 | |
| 7 | 3 | 0 | 3 | 25-27 | |
|
|
8 | 1 | 0 | 1 | 28 |
|
2 |
(9) |
|
2 |
(10) |
|
2 |
(11) |
|
2 |
(12) |
CONF
0 1 2 8 11 15
0 1 2 11 15 22
0 1 2 8 15 25
4 8 11 22 25 1 2 15
The complete data file for performing the
SCF and subsequent CI would then be as follows:
TITLE\N2 .. 4-31G*
SUPER OFF NOSYM
ZMAT ANGS\N\N 1 NN
VARIABLES\NN 1.05 \END
BASIS 4-31G*
RUNTYPE CI
MRDCI
TRAN CORE
1 0 0 0 1 0 0 0
1 1
SELECT
SINGLES 1
CONF
0 1 2 8 11 15
0 1 2 11 15 22
0 1 2 8 15 25
4 8 11 22 25 1 2 15
NATORB IPRIN
ENTER
Now consider the corresponding calculation performed in
a smaller 3-21G basis.
An examination of the SCF output
reveals the following orbital analysis.
=============================
IRREP NO. OF SYMMETRY ADAPTED
BASIS FUNCTIONS
=============================
1 5
2 2
3 2
5 5
6 2
7 2
=============================
and the following orbital assignments from
the converged closed shell SCF:
===============================================
M.O. IRREP ORBITAL ENERGY ORBITAL OCCUPANCY
===============================================
1 1 -15.59983859 2.0000000
2 5 -15.59796932 2.0000000
3 1 -1.54485796 2.0000000
4 5 -0.74550130 2.0000000
5 2 -0.63373069 2.0000000
6 3 -0.63373069 2.0000000
7 1 -0.62012170 2.0000000
8 6 0.20546760 0.0000000
9 7 0.20546760 0.0000000
10 5 0.79186362 0.0000000
11 1 1.16445455 0.0000000
12 2 1.26826720 0.0000000
13 3 1.26826720 0.0000000
14 7 1.43237859 0.0000000
15 6 1.43237859 0.0000000
16 5 1.55279124 0.0000000
17 1 1.83635478 0.0000000
18 5 2.63677794 0.0000000
===============================================
Note that there are now no MOs of IRREP 4 or 8.
Based on the above output, the CONF data lines may be
deduced from the following table, where we again
assume that we wish to freeze the two N1s inner shell orbitals:
| IRrep | IRrep | No. of Basis | Frozen | Active | Sequence |
| No. | Functions | MOs | MOs | Nos. | |
|
|
1 | 5 | 1 | 4 | 1-4 |
| 2 | 2 | 0 | 2 | 5-6 | |
| 3 | 2 | 0 | 2 | 7-8 | |
|
|
5 | 5 | 1 | 4 | 9-12 |
| 6 | 2 | 0 | 2 | 13-14 | |
| 7 | 2 | 0 | 2 | 15-16 |
CONF
0 1 2 5 7 9
The complete data file for performing the
SCF and subsequent CI would then be as follows:
TITLE\N2 .. 3-21G
SUPER OFF NOSYM
ZMAT ANGS\N\N 1 NN
VARIABLES\NN 1.05 \END
BASIS 3-21G
RUNTYPE CI
MRDCI
TRAN CORE
1 0 0 1 0 0
1 1
SELECT
SINGLES 1
CONF
0 1 2 5 7 9
NATORB IPRIN
ENTER
Example 5
In this example we wish to perform a valence-CI calculation
on the CaH2 molecule using a 3-21G basis. While the molecular symmetry
is D
h, the symmetry adaptation and subsequent CI
will be conducted in the
D2h point group. An examination of the SCF output
reveals the following orbital analysis.
=============================
IRREP NO. OF SYMMETRY ADAPTED
BASIS FUNCTIONS
=============================
1 7
2 4
3 4
5 6
=============================
and the following orbital assignments from
the converged closed shell SCF:
===============================================
M.O. IRREP ORBITAL ENERGY ORBITAL OCCUPANCY
===============================================
1 1 -148.37173884 2.0000000
2 1 -16.76521275 2.0000000
3 3 -13.55586861 2.0000000
4 2 -13.55586861 2.0000000
5 5 -13.55460610 2.0000000
6 1 -2.26357685 2.0000000
7 3 -1.36160958 2.0000000
8 2 -1.36160958 2.0000000
9 5 -1.35089927 2.0000000
10 1 -0.34923025 2.0000000
11 5 -0.31649941 2.0000000
12 2 0.02334207 0.0000000
13 3 0.02334207 0.0000000
14 1 0.04980631 0.0000000
15 5 0.09478404 0.0000000
16 1 0.12395484 0.0000000
17 3 0.13549605 0.0000000
18 2 0.13549605 0.0000000
19 5 0.28345574 0.0000000
20 1 1.32404002 0.0000000
21 5 1.45900204 0.0000000
===============================================
Based on the above output, the CONF data lines may be
deduced from the following table, where we
assume that we wish to freeze the nine Ca inner shell orbitals:
| IRrep | IRrep | No. of Basis | Frozen | Active | Sequence |
| No. | Functions | MOs | MOs | Nos. | |
|
|
1 | 7 | 3 | 4 | 1-4 |
| 2 | 4 | 2 | 2 | 5-6 | |
| 3 | 4 | 2 | 2 | 7-8 | |
|
|
5 | 6 | 2 | 4 | 9-12 |
CONF
0 1 9
The complete data file for performing the
SCF and subsequent CI would then be as follows:
TITLE\CAH2 .. 3-21G
SUPER OFF NOSYM
ZMAT ANGS\CA\X 1 1.0\ H 1 CAH 2 90.0\H 1 CAH 2 90.0 3 THETA
VARIABLES\CAH 2.148 \THETA 180.0 \END
BASIS 3-21G
RUNTYPE CI
MRDCI
TRAN CORE
3 2 2 2
1 2 3 1 2 1 2 1 2
SELECT
SINGLES 1
CONF
0 1 9
NATORB IPRIN
ENTER
The ROOTS directive is used to specify those eigenvectors of the `root' secular problem to be used in the process of selection, with the energy contributions of the configurations computed with respect to the nominated vectors. The directive consists of a single data line with the character string ROOTS in the first data field. Subsequent data comprises integer variables used to specify the number of root eigenstates (NROOT) and the sequence numbers of these vectors within the matrix of zero-order eigenvectors, (IROOT(I),I=1,NROOT). Two formats may be used in this specification:
ROOTS 1
Example
THRESH 5.0 5.0
THRESH 5 5
are equivalent, causing Tmin and Tinc to be set to
5 microhartree.