Reduction formula for point group S6
Characters for molecular motions
Motion |
E |
C3(z) |
(C3)2 |
i |
(S6)5 |
S6 |
Cartesian 3N |
54 |
0 |
0 |
0 |
0 |
0 |
Translation (x,y,z) |
3 |
0 |
0 |
-3 |
0 |
0 |
Rotation (Rx,Ry,Rz) |
3 |
0 |
0 |
3 |
0 |
0 |
Vibration |
48 |
0 |
0 |
0 |
0 |
0 |
Decomposition into Irreducible representations
Motion |
Ag |
Eg |
Au |
Eu |
Total |
Cartesian 3N |
9 |
9 |
9 |
9 |
36 |
Translation (x,y,z) |
0 |
0 |
1 |
1 |
2 |
Rotation (Rx,Ry,Rz) |
1 |
1 |
0 |
0 |
2 |
Vibration |
8 |
8 |
8 |
8 |
32 |
Molecule Parameter
Number of Atoms (N) |
18 |
Number of internal coordinates |
48 |
Number of independant internal coordinates |
8 |
Number of vibrational modes |
32 |
Force field analysis
Allowed / forbidden vibronational transitions
Operator |
Ag |
Eg |
Au |
Eu |
Total |
Linear (IR) |
8 |
8 |
8 |
8 |
16 / 16 |
Quadratic (Raman) |
8 |
8 |
8 |
8 |
16 / 16 |
IR + Raman |
- |
- |
- |
- |
0* / 0 |
* Center of inversion: Mutual Exclusion Principle
Characters of symmetric powers for vibration representation
Force field |
Tensor Order |
E |
C3(z) |
(C3)2 |
i |
(S6)5 |
S6 |
linear |
1 |
48 |
0 |
0 |
0 |
0 |
0 |
quadratic |
2 |
1.176 |
0 |
0 |
24 |
0 |
0 |
cubic |
3 |
19.600 |
16 |
16 |
0 |
0 |
0 |
quartic |
4 |
249.900 |
0 |
0 |
300 |
0 |
0 |
quintic |
5 |
2.598.960 |
0 |
0 |
0 |
0 |
0 |
sextic |
6 |
22.957.480 |
136 |
136 |
2.600 |
8 |
8 |
Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field |
Tensor Order |
Ag |
Eg |
Au |
Eu |
linear |
1 |
8 |
8 |
8 |
8 |
quadratic |
2 |
200 |
200 |
192 |
192 |
cubic |
3 |
3.272 |
3.264 |
3.272 |
3.264 |
quartic |
4 |
41.700 |
41.700 |
41.600 |
41.600 |
quintic |
5 |
433.160 |
433.160 |
433.160 |
433.160 |
sextic |
6 |
3.826.728 |
3.826.656 |
3.825.856 |
3.825.792 |
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