Reduction formula for point group Td
Characters for molecular motions
Motion |
E |
8C3 |
3C2 |
6S4 |
6d |
Cartesian 3N |
36 |
0 |
-4 |
0 |
4 |
Translation (x,y,z) |
3 |
0 |
-1 |
-1 |
1 |
Rotation (Rx,Ry,Rz) |
3 |
0 |
-1 |
1 |
-1 |
Vibration |
30 |
0 |
-2 |
0 |
4 |
Decomposition into Irreducible representations
Motion |
A1 |
A2 |
E |
T1 |
T2 |
Total |
Cartesian 3N |
2 |
0 |
2 |
4 |
6 |
14 |
Translation (x,y,z) |
0 |
0 |
0 |
0 |
1 |
1 |
Rotation (Rx,Ry,Rz) |
0 |
0 |
0 |
1 |
0 |
1 |
Vibration |
2 |
0 |
2 |
3 |
5 |
12 |
Molecule Parameter
Number of Atoms (N) |
12 |
Number of internal coordinates |
30 |
Number of independant internal coordinates |
2 |
Number of vibrational modes |
12 |
Force field analysis
Allowed / forbidden vibronational transitions
Operator |
A1 |
A2 |
E |
T1 |
T2 |
Total |
Linear (IR) |
2 |
0 |
2 |
3 |
5 |
5 / 7 |
Quadratic (Raman) |
2 |
0 |
2 |
3 |
5 |
9 / 3 |
IR + Raman |
- |
0 |
- |
3 |
5 |
5 / 3 |
Characters of symmetric powers for vibration representation
Force field |
Tensor Order |
E |
8C3 |
3C2 |
6S4 |
6d |
linear |
1 |
30 |
0 |
-2 |
0 |
4 |
quadratic |
2 |
465 |
0 |
17 |
-1 |
23 |
cubic |
3 |
4.960 |
10 |
-32 |
0 |
72 |
quartic |
4 |
40.920 |
0 |
152 |
8 |
256 |
quintic |
5 |
278.256 |
0 |
-272 |
0 |
680 |
sextic |
6 |
1.623.160 |
55 |
952 |
-8 |
1.904 |
Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field |
Tensor Order |
A1 |
A2 |
E |
T1 |
T2 |
linear |
1 |
2 |
0 |
2 |
3 |
5 |
quadratic |
2 |
27 |
16 |
43 |
50 |
62 |
cubic |
3 |
224 |
188 |
402 |
606 |
642 |
quartic |
4 |
1.790 |
1.658 |
3.448 |
5.034 |
5.158 |
quintic |
5 |
11.730 |
11.390 |
23.120 |
34.646 |
34.986 |
sextic |
6 |
68.243 |
67.295 |
135.483 |
202.298 |
203.254 |
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