Reduction formula for point group D4h
Characters for molecular motions
Motion |
E |
2C4 (z) |
C2 |
2C'2 |
2C''2 |
i |
2S4 |
h |
2v |
2d |
Cartesian 3N |
156 |
0 |
0 |
0 |
-2 |
0 |
0 |
4 |
4 |
14 |
Translation (x,y,z) |
3 |
1 |
-1 |
-1 |
-1 |
-3 |
-1 |
1 |
1 |
1 |
Rotation (Rx,Ry,Rz) |
3 |
1 |
-1 |
-1 |
-1 |
3 |
1 |
-1 |
-1 |
-1 |
Vibration |
150 |
-2 |
2 |
2 |
0 |
0 |
0 |
4 |
4 |
14 |
Decomposition into Irreducible representations
Motion |
A1g |
A2g |
B1g |
B2g |
Eg |
A1u |
A2u |
B1u |
B2u |
Eu |
Total |
Cartesian 3N |
12 |
8 |
9 |
11 |
19 |
7 |
12 |
11 |
8 |
20 |
117 |
Translation (x,y,z) |
0 |
0 |
0 |
0 |
0 |
0 |
1 |
0 |
0 |
1 |
2 |
Rotation (Rx,Ry,Rz) |
0 |
1 |
0 |
0 |
1 |
0 |
0 |
0 |
0 |
0 |
2 |
Vibration |
12 |
7 |
9 |
11 |
18 |
7 |
11 |
11 |
8 |
19 |
113 |
Molecule Parameter
Number of Atoms (N) |
52 |
Number of internal coordinates |
150 |
Number of independant internal coordinates |
12 |
Number of vibrational modes |
113 |
Force field analysis
Allowed / forbidden vibronational transitions
Operator |
A1g |
A2g |
B1g |
B2g |
Eg |
A1u |
A2u |
B1u |
B2u |
Eu |
Total |
Linear (IR) |
12 |
7 |
9 |
11 |
18 |
7 |
11 |
11 |
8 |
19 |
30 / 83 |
Quadratic (Raman) |
12 |
7 |
9 |
11 |
18 |
7 |
11 |
11 |
8 |
19 |
50 / 63 |
IR + Raman |
- |
7 |
- |
- |
- |
7 |
- |
11 |
8 |
- |
0* / 33 |
* Center of inversion: Mutual Exclusion Principle
Characters of symmetric powers for vibration representation
Force field |
Tensor Order |
E |
2C4 (z) |
C2 |
2C'2 |
2C''2 |
i |
2S4 |
h |
2v |
2d |
linear |
1 |
150 |
-2 |
2 |
2 |
0 |
0 |
0 |
4 |
4 |
14 |
quadratic |
2 |
11.325 |
3 |
77 |
77 |
75 |
75 |
1 |
83 |
83 |
173 |
cubic |
3 |
573.800 |
-4 |
152 |
152 |
0 |
0 |
0 |
312 |
312 |
1.512 |
quartic |
4 |
21.947.850 |
42 |
3.002 |
3.002 |
2.850 |
2.850 |
38 |
3.466 |
3.466 |
11.866 |
quintic |
5 |
675.993.780 |
-80 |
5.852 |
5.852 |
0 |
0 |
0 |
12.320 |
12.320 |
79.492 |
sextic |
6 |
17.463.172.650 |
118 |
79.002 |
79.002 |
73.150 |
73.150 |
38 |
97.174 |
97.174 |
490.042 |
Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field |
Tensor Order |
A1g |
A2g |
B1g |
B2g |
Eg |
A1u |
A2u |
B1u |
B2u |
Eu |
linear |
1 |
12 |
7 |
9 |
11 |
18 |
7 |
11 |
11 |
8 |
19 |
quadratic |
2 |
774 |
672 |
711 |
733 |
1.405 |
690 |
716 |
714 |
691 |
1.407 |
cubic |
3 |
36.138 |
35.644 |
35.761 |
36.023 |
71.667 |
35.643 |
36.061 |
36.022 |
35.684 |
71.745 |
quartic |
4 |
1.374.981 |
1.369.685 |
1.371.282 |
1.373.344 |
2.743.029 |
1.370.349 |
1.372.719 |
1.372.602 |
1.370.464 |
2.743.183 |
quintic |
5 |
42.262.945 |
42.238.529 |
42.243.092 |
42.258.422 |
84.496.951 |
42.238.452 |
42.259.942 |
42.258.345 |
42.240.089 |
84.500.031 |
sextic |
6 |
1.091.556.314 |
1.091.371.472 |
1.091.415.477 |
1.091.512.231 |
2.182.883.703 |
1.091.388.210 |
1.091.496.976 |
1.091.492.413 |
1.091.392.733 |
2.182.889.709 |
Literature
- J.K.G. Watson, J. Mol. Spec. 41 229 (1972)
The Numbers of Structural Parameters and Potential Constants of Molecules
- X.F. Zhou, P. Pulay. J. Comp. Chem. 10 No. 7, 935-938 (1989)
Characters for Symmetric and Antisymmetric Higher Powers of Representations:
Application to the Number of Anharmonic Force Constants in Symmetrical Molecules
Last update November, 13th 2023 by A. Gelessus, Impressum, Datenschutzerklärung/DataPrivacyStatement