Reduction formula for point group C3v
Characters for molecular motions
Motion |
E |
2C3 (z) |
3v |
Cartesian 3N |
216 |
0 |
0 |
Translation (x,y,z) |
3 |
0 |
1 |
Rotation (Rx,Ry,Rz) |
3 |
0 |
-1 |
Vibration |
210 |
0 |
0 |
Decomposition into Irreducible representations
Motion |
A1 |
A2 |
E |
Total |
Cartesian 3N |
36 |
36 |
72 |
144 |
Translation (x,y,z) |
1 |
0 |
1 |
2 |
Rotation (Rx,Ry,Rz) |
0 |
1 |
1 |
2 |
Vibration |
35 |
35 |
70 |
140 |
Molecule Parameter
Number of Atoms (N) |
72 |
Number of internal coordinates |
210 |
Number of independant internal coordinates |
35 |
Number of vibrational modes |
140 |
Force field analysis
Allowed / forbidden vibronational transitions
Operator |
A1 |
A2 |
E |
Total |
Linear (IR) |
35 |
35 |
70 |
105 / 35 |
Quadratic (Raman) |
35 |
35 |
70 |
105 / 35 |
IR + Raman |
35 |
35 |
70 |
105 / 35 |
Characters of symmetric powers for vibration representation
Force field |
Tensor Order |
E |
2C3 (z) |
3v |
linear |
1 |
210 |
0 |
0 |
quadratic |
2 |
22.155 |
0 |
105 |
cubic |
3 |
1.565.620 |
70 |
0 |
quartic |
4 |
83.369.265 |
0 |
5.565 |
quintic |
5 |
3.568.204.542 |
0 |
0 |
sextic |
6 |
127.860.662.755 |
2.485 |
198.485 |
Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field |
Tensor Order |
A1 |
A2 |
E |
linear |
1 |
35 |
35 |
70 |
quadratic |
2 |
3.745 |
3.640 |
7.385 |
cubic |
3 |
260.960 |
260.960 |
521.850 |
quartic |
4 |
13.897.660 |
13.892.095 |
27.789.755 |
quintic |
5 |
594.700.757 |
594.700.757 |
1.189.401.514 |
sextic |
6 |
21.310.210.530 |
21.310.012.045 |
42.620.220.090 |
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