Reduction formula for point group C3v
Characters for molecular motions
| Motion |
E |
2C3 (z) |
3 v |
| Cartesian 3N |
21 |
0 |
3 |
| Translation (x,y,z) |
3 |
0 |
1 |
| Rotation (Rx,Ry,Rz) |
3 |
0 |
-1 |
| Vibration |
15 |
0 |
3 |
Decomposition into Irreducible representations
| Motion |
A1 |
A2 |
E |
Total |
| Cartesian 3N |
5 |
2 |
7 |
14 |
| Translation (x,y,z) |
1 |
0 |
1 |
2 |
| Rotation (Rx,Ry,Rz) |
0 |
1 |
1 |
2 |
| Vibration |
4 |
1 |
5 |
10 |
Molecule Parameter
| Number of Atoms (N) |
7 |
| Number of internal coordinates |
15 |
| Number of independant internal coordinates |
4 |
| Number of vibrational modes |
10 |
Force field analysis
Allowed / forbidden vibronational transitions
| Operator |
A1 |
A2 |
E |
Total |
| Linear (IR) |
4 |
1 |
5 |
9 / 1 |
| Quadratic (Raman) |
4 |
1 |
5 |
9 / 1 |
| IR + Raman |
4 |
1 |
5 |
9 / 1 |
Characters of symmetric powers for vibration representation
| Force field |
Tensor
Order |
E |
2C3 (z) |
3v |
| linear |
1 |
15 |
0 |
3 |
| quadratic |
2 |
120 |
0 |
12 |
| cubic |
3 |
680 |
5 |
28 |
| quartic |
4 |
3.060 |
0 |
72 |
| quintic |
5 |
11.628 |
0 |
144 |
| sextic |
6 |
38.760 |
15 |
300 |
Decomposition into Irreducible representations
Number of nonvanshing force constants
| Force field |
Tensor
Order |
A1 |
A2 |
E |
| linear |
1 |
4 |
1 |
5 |
| quadratic |
2 |
26 |
14 |
40 |
| cubic |
3 |
129 |
101 |
225 |
| quartic |
4 |
546 |
474 |
1.020 |
| quintic |
5 |
2.010 |
1.866 |
3.876 |
| sextic |
6 |
6.615 |
6.315 |
12.915 |
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