Reduction formula for point group C3h
Characters for molecular motions
Motion |
E |
C3(z) |
(C3)2 |
h |
S3 |
(S3)5 |
Cartesian 3N |
324 |
0 |
0 |
24 |
0 |
0 |
Translation (x,y,z) |
3 |
0 |
0 |
1 |
-2 |
-2 |
Rotation (Rx,Ry,Rz) |
3 |
0 |
0 |
-1 |
2 |
2 |
Vibration |
318 |
0 |
0 |
24 |
0 |
0 |
Decomposition into Irreducible representations
Motion |
A' |
E' |
A'' |
E'' |
Total |
Cartesian 3N |
58 |
58 |
50 |
50 |
216 |
Translation (x,y,z) |
0 |
1 |
1 |
0 |
2 |
Rotation (Rx,Ry,Rz) |
1 |
0 |
0 |
1 |
2 |
Vibration |
57 |
57 |
49 |
49 |
212 |
Molecule Parameter
Number of Atoms (N) |
108 |
Number of internal coordinates |
318 |
Number of independant internal coordinates |
57 |
Number of vibrational modes |
212 |
Force field analysis
Allowed / forbidden vibronational transitions
Operator |
A' |
E' |
A'' |
E'' |
Total |
Linear (IR) |
57 |
57 |
49 |
49 |
106 / 106 |
Quadratic (Raman) |
57 |
57 |
49 |
49 |
163 / 49 |
IR + Raman |
- |
57 |
- |
- |
57 / 0 |
Characters of symmetric powers for vibration representation
Force field |
Tensor Order |
E |
C3(z) |
(C3)2 |
h |
S3 |
(S3)5 |
linear |
1 |
318 |
0 |
0 |
24 |
0 |
0 |
quadratic |
2 |
50.721 |
0 |
0 |
447 |
0 |
0 |
cubic |
3 |
5.410.240 |
106 |
106 |
6.128 |
8 |
8 |
quartic |
4 |
434.171.760 |
0 |
0 |
72.528 |
0 |
0 |
quintic |
5 |
27.960.661.344 |
0 |
0 |
741.552 |
0 |
0 |
sextic |
6 |
1.505.215.602.352 |
5.671 |
5.671 |
6.858.544 |
85 |
85 |
Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field |
Tensor Order |
A' |
E' |
A'' |
E'' |
linear |
1 |
57 |
57 |
49 |
49 |
quadratic |
2 |
8.528 |
8.528 |
8.379 |
8.379 |
cubic |
3 |
902.766 |
902.709 |
900.718 |
900.669 |
quartic |
4 |
72.374.048 |
72.374.048 |
72.349.872 |
72.349.872 |
quintic |
5 |
4.660.233.816 |
4.660.233.816 |
4.659.986.632 |
4.659.986.632 |
sextic |
6 |
250.870.412.068 |
250.870.409.190 |
250.868.125.830 |
250.868.123.037 |
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