Reduction formula for point group C3
Characters for molecular motions
Motion |
E |
C3 |
(C3)2 |
Cartesian 3N |
63 |
0 |
0 |
Translation (x,y,z) |
3 |
0 |
0 |
Rotation (Rx,Ry,Rz) |
3 |
0 |
0 |
Vibration |
57 |
0 |
0 |
Decomposition into Irreducible representations
Motion |
A |
E |
Total |
Cartesian 3N |
21 |
21 |
42 |
Translation (x,y,z) |
1 |
1 |
2 |
Rotation (Rx,Ry,Rz) |
1 |
1 |
2 |
Vibration |
19 |
19 |
38 |
Molecule Parameter
Number of Atoms (N) |
21 |
Number of internal coordinates |
57 |
Number of independant internal coordinates |
19 |
Number of vibrational modes |
38 |
Force field analysis
Allowed / forbidden vibronational transitions
Operator |
A |
E |
Total |
Linear (IR) |
19 |
19 |
38 / 0 |
Quadratic (Raman) |
19 |
19 |
38 / 0 |
IR + Raman |
19 |
19 |
38 / 0 |
Characters of symmetric powers for vibration representation
Force field |
Tensor Order |
E |
C3 |
(C3)2 |
linear |
1 |
57 |
0 |
0 |
quadratic |
2 |
1.653 |
0 |
0 |
cubic |
3 |
32.509 |
19 |
19 |
quartic |
4 |
487.635 |
0 |
0 |
quintic |
5 |
5.949.147 |
0 |
0 |
sextic |
6 |
61.474.519 |
190 |
190 |
Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field |
Tensor Order |
A |
E |
linear |
1 |
19 |
19 |
quadratic |
2 |
551 |
551 |
cubic |
3 |
10.849 |
10.830 |
quartic |
4 |
162.545 |
162.545 |
quintic |
5 |
1.983.049 |
1.983.049 |
sextic |
6 |
20.491.633 |
20.491.443 |
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