Reduction formula for point group C3v
Characters for molecular motions
Motion |
E |
2C3 (z) |
3v |
Cartesian 3N |
144 |
0 |
8 |
Translation (x,y,z) |
3 |
0 |
1 |
Rotation (Rx,Ry,Rz) |
3 |
0 |
-1 |
Vibration |
138 |
0 |
8 |
Decomposition into Irreducible representations
Motion |
A1 |
A2 |
E |
Total |
Cartesian 3N |
28 |
20 |
48 |
96 |
Translation (x,y,z) |
1 |
0 |
1 |
2 |
Rotation (Rx,Ry,Rz) |
0 |
1 |
1 |
2 |
Vibration |
27 |
19 |
46 |
92 |
Molecule Parameter
Number of Atoms (N) |
48 |
Number of internal coordinates |
138 |
Number of independant internal coordinates |
27 |
Number of vibrational modes |
92 |
Force field analysis
Allowed / forbidden vibronational transitions
Operator |
A1 |
A2 |
E |
Total |
Linear (IR) |
27 |
19 |
46 |
73 / 19 |
Quadratic (Raman) |
27 |
19 |
46 |
73 / 19 |
IR + Raman |
27 |
19 |
46 |
73 / 19 |
Characters of symmetric powers for vibration representation
Force field |
Tensor Order |
E |
2C3 (z) |
3v |
linear |
1 |
138 |
0 |
8 |
quadratic |
2 |
9.591 |
0 |
101 |
cubic |
3 |
447.580 |
46 |
640 |
quartic |
4 |
15.777.195 |
0 |
4.815 |
quintic |
5 |
448.072.338 |
0 |
25.752 |
sextic |
6 |
10.679.057.389 |
1.081 |
148.291 |
Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field |
Tensor Order |
A1 |
A2 |
E |
linear |
1 |
27 |
19 |
46 |
quadratic |
2 |
1.649 |
1.548 |
3.197 |
cubic |
3 |
74.932 |
74.292 |
149.178 |
quartic |
4 |
2.631.940 |
2.627.125 |
5.259.065 |
quintic |
5 |
74.691.599 |
74.665.847 |
149.357.446 |
sextic |
6 |
1.779.917.404 |
1.779.769.113 |
3.559.685.436 |
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