Reduction formula for point group O
Characters for molecular motions
Motion |
E |
8C3 |
6C'2 |
6C4 |
3C2 =(C4)2 |
Cartesian 3N |
39 |
0 |
-1 |
5 |
-5 |
Translation (x,y,z) |
3 |
0 |
-1 |
1 |
-1 |
Rotation (Rx,Ry,Rz) |
3 |
0 |
-1 |
1 |
-1 |
Vibration |
33 |
0 |
1 |
3 |
-3 |
Decomposition into Irreducible representations
Motion |
A1 |
A2 |
E |
T1 |
T2 |
Total |
Cartesian 3N |
2 |
0 |
2 |
7 |
4 |
15 |
Translation (x,y,z) |
0 |
0 |
0 |
1 |
0 |
1 |
Rotation (Rx,Ry,Rz) |
0 |
0 |
0 |
1 |
0 |
1 |
Vibration |
2 |
0 |
2 |
5 |
4 |
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 |
A1 |
A2 |
E |
T1 |
T2 |
Total |
Linear (IR) |
2 |
0 |
2 |
5 |
4 |
5 / 8 |
Quadratic (Raman) |
2 |
0 |
2 |
5 |
4 |
8 / 5 |
IR + Raman |
- |
0 |
- |
- |
- |
0 / 0 |
Characters of symmetric powers for vibration representation
Force field |
Tensor Order |
E |
8C3 |
6C'2 |
6C4 |
3C2 =(C4)2 |
linear |
1 |
33 |
0 |
1 |
3 |
-3 |
quadratic |
2 |
561 |
0 |
17 |
3 |
21 |
cubic |
3 |
6.545 |
11 |
17 |
1 |
-55 |
quartic |
4 |
58.905 |
0 |
153 |
9 |
225 |
quintic |
5 |
435.897 |
0 |
153 |
27 |
-531 |
sextic |
6 |
2.760.681 |
66 |
969 |
27 |
1.653 |
Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field |
Tensor Order |
A1 |
A2 |
E |
T1 |
T2 |
linear |
1 |
2 |
0 |
2 |
5 |
4 |
quadratic |
2 |
31 |
21 |
52 |
64 |
71 |
cubic |
3 |
274 |
265 |
528 |
821 |
829 |
quartic |
4 |
2.523 |
2.442 |
4.965 |
7.299 |
7.371 |
quintic |
5 |
18.141 |
18.051 |
36.192 |
54.522 |
54.585 |
sextic |
6 |
115.506 |
115.008 |
230.448 |
344.643 |
345.114 |
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