Reduction formula for point group Oh
Characters for molecular motions
Motion |
E |
8C3 |
6C2 |
6C4 |
3C2 =(C4)2 |
i |
6S4 |
8S6 |
3h |
6d |
Cartesian 3N |
39 |
0 |
-1 |
5 |
-5 |
-3 |
-1 |
0 |
9 |
5 |
Translation (x,y,z) |
3 |
0 |
-1 |
1 |
-1 |
-3 |
-1 |
0 |
1 |
1 |
Rotation (Rx,Ry,Rz) |
3 |
0 |
-1 |
1 |
-1 |
3 |
1 |
0 |
-1 |
-1 |
Vibration |
33 |
0 |
1 |
3 |
-3 |
-3 |
-1 |
0 |
9 |
5 |
Decomposition into Irreducible representations
Motion |
A1g |
A2g |
Eg |
T1g |
T2g |
A1u |
A2u |
Eu |
T1u |
T2u |
Total |
Cartesian 3N |
2 |
0 |
2 |
2 |
2 |
0 |
0 |
0 |
5 |
2 |
15 |
Translation (x,y,z) |
0 |
0 |
0 |
0 |
0 |
0 |
0 |
0 |
1 |
0 |
1 |
Rotation (Rx,Ry,Rz) |
0 |
0 |
0 |
1 |
0 |
0 |
0 |
0 |
0 |
0 |
1 |
Vibration |
2 |
0 |
2 |
1 |
2 |
0 |
0 |
0 |
4 |
2 |
13 |
Molecule Parameter
Number of Atoms (N) |
13 |
Number of internal coordinates |
33 |
Number of independant internal coordinates |
2 |
Number of vibrational modes |
13 |
Force field analysis
Allowed / forbidden vibronational transitions
Operator |
A1g |
A2g |
Eg |
T1g |
T2g |
A1u |
A2u |
Eu |
T1u |
T2u |
Total |
Linear (IR) |
2 |
0 |
2 |
1 |
2 |
0 |
0 |
0 |
4 |
2 |
4 / 9 |
Quadratic (Raman) |
2 |
0 |
2 |
1 |
2 |
0 |
0 |
0 |
4 |
2 |
6 / 7 |
IR + Raman |
- |
0 |
- |
1 |
- |
0 |
0 |
0 |
- |
2 |
0* / 3 |
* Center of inversion: Mutual Exclusion Principle
Characters of symmetric powers for vibration representation
Force field |
Tensor Order |
E |
8C3 |
6C2 |
6C4 |
3C2 =(C4)2 |
i |
6S4 |
8S6 |
3h |
6d |
linear |
1 |
33 |
0 |
1 |
3 |
-3 |
-3 |
-1 |
0 |
9 |
5 |
quadratic |
2 |
561 |
0 |
17 |
3 |
21 |
21 |
-1 |
0 |
57 |
29 |
cubic |
3 |
6.545 |
11 |
17 |
1 |
-55 |
-55 |
1 |
-1 |
273 |
105 |
quartic |
4 |
58.905 |
0 |
153 |
9 |
225 |
225 |
9 |
0 |
1.113 |
385 |
quintic |
5 |
435.897 |
0 |
153 |
27 |
-531 |
-531 |
-9 |
0 |
3.969 |
1.141 |
sextic |
6 |
2.760.681 |
66 |
969 |
27 |
1.653 |
1.653 |
-9 |
6 |
12.817 |
3.325 |
Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field |
Tensor Order |
A1g |
A2g |
Eg |
T1g |
T2g |
A1u |
A2u |
Eu |
T1u |
T2u |
linear |
1 |
2 |
0 |
2 |
1 |
2 |
0 |
0 |
0 |
4 |
2 |
quadratic |
2 |
23 |
11 |
34 |
26 |
37 |
8 |
10 |
18 |
38 |
34 |
cubic |
3 |
166 |
135 |
296 |
377 |
407 |
108 |
130 |
232 |
444 |
422 |
quartic |
4 |
1.385 |
1.246 |
2.631 |
3.547 |
3.677 |
1.138 |
1.196 |
2.334 |
3.752 |
3.694 |
quintic |
5 |
9.449 |
9.121 |
18.570 |
26.836 |
27.155 |
8.692 |
8.930 |
17.622 |
27.686 |
27.430 |
sextic |
6 |
59.004 |
57.926 |
116.894 |
171.207 |
172.276 |
56.502 |
57.082 |
113.554 |
173.436 |
172.838 |
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