Reduction formula for point group Td
Characters for molecular motions
| Motion |
E |
8C3 |
3C2 |
6S4 |
6 d |
| Cartesian 3N |
30 |
0 |
-2 |
0 |
4 |
| Translation (x,y,z) |
3 |
0 |
-1 |
-1 |
1 |
| Rotation (Rx,Ry,Rz) |
3 |
0 |
-1 |
1 |
-1 |
| Vibration |
24 |
0 |
0 |
0 |
4 |
Decomposition into Irreducible representations
| Motion |
A1 |
A2 |
E |
T1 |
T2 |
Total |
| Cartesian 3N |
2 |
0 |
2 |
3 |
5 |
12 |
| Translation (x,y,z) |
0 |
0 |
0 |
0 |
1 |
1 |
| Rotation (Rx,Ry,Rz) |
0 |
0 |
0 |
1 |
0 |
1 |
| Vibration |
2 |
0 |
2 |
2 |
4 |
10 |
Molecule Parameter
| Number of Atoms (N) |
10 |
| Number of internal coordinates |
24 |
| Number of independant internal coordinates |
2 |
| Number of vibrational modes |
10 |
Force field analysis
Allowed / forbidden vibronational transitions
| Operator |
A1 |
A2 |
E |
T1 |
T2 |
Total |
| Linear (IR) |
2 |
0 |
2 |
2 |
4 |
4 / 6 |
| Quadratic (Raman) |
2 |
0 |
2 |
2 |
4 |
8 / 2 |
| IR + Raman |
- |
0 |
- |
2 |
4 |
4 / 2 |
Characters of symmetric powers for vibration representation
| Force field |
Tensor
Order |
E |
8C3 |
3C2 |
6S4 |
6d |
| linear |
1 |
24 |
0 |
0 |
0 |
4 |
| quadratic |
2 |
300 |
0 |
12 |
0 |
20 |
| cubic |
3 |
2.600 |
8 |
0 |
0 |
60 |
| quartic |
4 |
17.550 |
0 |
78 |
6 |
190 |
| quintic |
5 |
98.280 |
0 |
0 |
0 |
476 |
| sextic |
6 |
475.020 |
36 |
364 |
0 |
1.204 |
Decomposition into Irreducible representations
Number of nonvanshing force constants
| Force field |
Tensor
Order |
A1 |
A2 |
E |
T1 |
T2 |
| linear |
1 |
2 |
0 |
2 |
2 |
4 |
| quadratic |
2 |
19 |
9 |
28 |
31 |
41 |
| cubic |
3 |
126 |
96 |
214 |
310 |
340 |
| quartic |
4 |
790 |
692 |
1.482 |
2.138 |
2.230 |
| quintic |
5 |
4.214 |
3.976 |
8.190 |
12.166 |
12.404 |
| sextic |
6 |
20.151 |
19.549 |
39.664 |
59.031 |
59.633 |
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