Reduction formula for point group S6
Characters for molecular motions
Motion |
E |
C3(z) |
(C3)2 |
i |
(S6)5 |
S6 |
Cartesian 3N |
48 |
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 |
42 |
0 |
0 |
0 |
0 |
0 |
Decomposition into Irreducible representations
Motion |
Ag |
Eg |
Au |
Eu |
Total |
Cartesian 3N |
8 |
8 |
8 |
8 |
32 |
Translation (x,y,z) |
0 |
0 |
1 |
1 |
2 |
Rotation (Rx,Ry,Rz) |
1 |
1 |
0 |
0 |
2 |
Vibration |
7 |
7 |
7 |
7 |
28 |
Molecule Parameter
Number of Atoms (N) |
16 |
Number of internal coordinates |
42 |
Number of independant internal coordinates |
7 |
Number of vibrational modes |
28 |
Force field analysis
Allowed / forbidden vibronational transitions
Operator |
Ag |
Eg |
Au |
Eu |
Total |
Linear (IR) |
7 |
7 |
7 |
7 |
14 / 14 |
Quadratic (Raman) |
7 |
7 |
7 |
7 |
14 / 14 |
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 |
42 |
0 |
0 |
0 |
0 |
0 |
quadratic |
2 |
903 |
0 |
0 |
21 |
0 |
0 |
cubic |
3 |
13.244 |
14 |
14 |
0 |
0 |
0 |
quartic |
4 |
148.995 |
0 |
0 |
231 |
0 |
0 |
quintic |
5 |
1.370.754 |
0 |
0 |
0 |
0 |
0 |
sextic |
6 |
10.737.573 |
105 |
105 |
1.771 |
7 |
7 |
Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field |
Tensor Order |
Ag |
Eg |
Au |
Eu |
linear |
1 |
7 |
7 |
7 |
7 |
quadratic |
2 |
154 |
154 |
147 |
147 |
cubic |
3 |
2.212 |
2.205 |
2.212 |
2.205 |
quartic |
4 |
24.871 |
24.871 |
24.794 |
24.794 |
quintic |
5 |
228.459 |
228.459 |
228.459 |
228.459 |
sextic |
6 |
1.789.928 |
1.789.872 |
1.789.333 |
1.789.284 |
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