Reduction formula for point group C3v
Characters for molecular motions
Motion |
E |
2C3 (z) |
3v |
Cartesian 3N |
12 |
0 |
2 |
Translation (x,y,z) |
3 |
0 |
1 |
Rotation (Rx,Ry,Rz) |
3 |
0 |
-1 |
Vibration |
6 |
0 |
2 |
Decomposition into Irreducible representations
Motion |
A1 |
A2 |
E |
Total |
Cartesian 3N |
3 |
1 |
4 |
8 |
Translation (x,y,z) |
1 |
0 |
1 |
2 |
Rotation (Rx,Ry,Rz) |
0 |
1 |
1 |
2 |
Vibration |
2 |
0 |
2 |
4 |
Molecule Parameter
Number of Atoms (N) |
4 |
Number of internal coordinates |
6 |
Number of independant internal coordinates |
2 |
Number of vibrational modes |
4 |
Force field analysis
Allowed / forbidden vibronational transitions
Operator |
A1 |
A2 |
E |
Total |
Linear (IR) |
2 |
0 |
2 |
4 / 0 |
Quadratic (Raman) |
2 |
0 |
2 |
4 / 0 |
IR + Raman |
2 |
0 |
2 |
4 / 0 |
Characters of symmetric powers for vibration representation
Force field |
Tensor Order |
E |
2C3 (z) |
3v |
linear |
1 |
6 |
0 |
2 |
quadratic |
2 |
21 |
0 |
5 |
cubic |
3 |
56 |
2 |
8 |
quartic |
4 |
126 |
0 |
14 |
quintic |
5 |
252 |
0 |
20 |
sextic |
6 |
462 |
3 |
30 |
Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field |
Tensor Order |
A1 |
A2 |
E |
linear |
1 |
2 |
0 |
2 |
quadratic |
2 |
6 |
1 |
7 |
cubic |
3 |
14 |
6 |
18 |
quartic |
4 |
28 |
14 |
42 |
quintic |
5 |
52 |
32 |
84 |
sextic |
6 |
93 |
63 |
153 |
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