Reduction formula for point group C2h
Characters for molecular motions
| Motion |
E |
C2 (z) |
i |
 h |
| Cartesian 3N |
108 |
-4 |
0 |
0 |
| Translation (x,y,z) |
3 |
-1 |
-3 |
1 |
| Rotation (Rx,Ry,Rz) |
3 |
-1 |
3 |
-1 |
| Vibration |
102 |
-2 |
0 |
0 |
Decomposition into Irreducible representations
| Motion |
Ag |
Bg |
Au |
Bu |
Total |
| Cartesian 3N |
26 |
28 |
26 |
28 |
108 |
| Translation (x,y,z) |
0 |
0 |
1 |
2 |
3 |
| Rotation (Rx,Ry,Rz) |
1 |
2 |
0 |
0 |
3 |
| Vibration |
25 |
26 |
25 |
26 |
102 |
Molecule Parameter
| Number of Atoms (N) |
36 |
| Number of internal coordinates |
102 |
| Number of independant internal coordinates |
25 |
| Number of vibrational modes |
102 |
Force field analysis
Allowed / forbidden vibronational transitions
| Operator |
Ag |
Bg |
Au |
Bu |
Total |
| Linear (IR) |
25 |
26 |
25 |
26 |
51 / 51 |
| Quadratic (Raman) |
25 |
26 |
25 |
26 |
51 / 51 |
| IR + Raman |
- |
- |
- |
- |
0* / 0 |
* Center of inversion: Mutual Exclusion Principle
Characters of symmetric powers for vibration representation
| Force field |
Tensor
Order |
E |
C2 (z) |
i |
h |
| linear |
1 |
102 |
-2 |
0 |
0 |
| quadratic |
2 |
5.253 |
53 |
51 |
51 |
| cubic |
3 |
182.104 |
-104 |
0 |
0 |
| quartic |
4 |
4.780.230 |
1.430 |
1.326 |
1.326 |
| quintic |
5 |
101.340.876 |
-2.756 |
0 |
0 |
| sextic |
6 |
1.807.245.622 |
26.182 |
23.426 |
23.426 |
Decomposition into Irreducible representations
Number of nonvanshing force constants
| Force field |
Tensor
Order |
Ag |
Bg |
Au |
Bu |
| linear |
1 |
25 |
26 |
25 |
26 |
| quadratic |
2 |
1.352 |
1.300 |
1.301 |
1.300 |
| cubic |
3 |
45.500 |
45.552 |
45.500 |
45.552 |
| quartic |
4 |
1.196.078 |
1.194.700 |
1.194.752 |
1.194.700 |
| quintic |
5 |
25.334.530 |
25.335.908 |
25.334.530 |
25.335.908 |
| sextic |
6 |
451.829.664 |
451.804.860 |
451.806.238 |
451.804.860 |
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