Reduction formula for point group Td
Characters for molecular motions
Motion |
E |
8C3 |
3C2 |
6S4 |
6d |
Cartesian 3N |
51 |
0 |
-1 |
-1 |
5 |
Translation (x,y,z) |
3 |
0 |
-1 |
-1 |
1 |
Rotation (Rx,Ry,Rz) |
3 |
0 |
-1 |
1 |
-1 |
Vibration |
45 |
0 |
1 |
-1 |
5 |
Decomposition into Irreducible representations
Motion |
A1 |
A2 |
E |
T1 |
T2 |
Total |
Cartesian 3N |
3 |
1 |
4 |
5 |
8 |
21 |
Translation (x,y,z) |
0 |
0 |
0 |
0 |
1 |
1 |
Rotation (Rx,Ry,Rz) |
0 |
0 |
0 |
1 |
0 |
1 |
Vibration |
3 |
1 |
4 |
4 |
7 |
19 |
Molecule Parameter
Number of Atoms (N) |
17 |
Number of internal coordinates |
45 |
Number of independant internal coordinates |
3 |
Number of vibrational modes |
19 |
Force field analysis
Allowed / forbidden vibronational transitions
Operator |
A1 |
A2 |
E |
T1 |
T2 |
Total |
Linear (IR) |
3 |
1 |
4 |
4 |
7 |
7 / 12 |
Quadratic (Raman) |
3 |
1 |
4 |
4 |
7 |
14 / 5 |
IR + Raman |
- |
1 |
- |
4 |
7 |
7 / 5 |
Characters of symmetric powers for vibration representation
Force field |
Tensor Order |
E |
8C3 |
3C2 |
6S4 |
6d |
linear |
1 |
45 |
0 |
1 |
-1 |
5 |
quadratic |
2 |
1.035 |
0 |
23 |
1 |
35 |
cubic |
3 |
16.215 |
15 |
23 |
-1 |
135 |
quartic |
4 |
194.580 |
0 |
276 |
12 |
580 |
quintic |
5 |
1.906.884 |
0 |
276 |
-12 |
1.876 |
sextic |
6 |
15.890.700 |
120 |
2.300 |
12 |
6.300 |
Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field |
Tensor Order |
A1 |
A2 |
E |
T1 |
T2 |
linear |
1 |
3 |
1 |
4 |
4 |
7 |
quadratic |
2 |
55 |
37 |
92 |
118 |
135 |
cubic |
3 |
717 |
650 |
1.352 |
1.990 |
2.058 |
quartic |
4 |
8.290 |
7.994 |
16.284 |
24.146 |
24.430 |
quintic |
5 |
79.954 |
79.022 |
158.976 |
237.854 |
238.798 |
sextic |
6 |
664.018 |
660.862 |
1.324.760 |
1.984.478 |
1.987.622 |
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