Reduction formula for point group D3d
Characters for molecular motions
Motion |
E |
2C3 |
3C'2 |
i |
2S6 |
3d |
Cartesian 3N |
21 |
0 |
-1 |
-3 |
0 |
3 |
Translation (x,y,z) |
3 |
0 |
-1 |
-3 |
0 |
1 |
Rotation (Rx,Ry,Rz) |
3 |
0 |
-1 |
3 |
0 |
-1 |
Vibration |
15 |
0 |
1 |
-3 |
0 |
3 |
Decomposition into Irreducible representations
Motion |
A1g |
A2g |
Eg |
A1u |
A2u |
Eu |
Total |
Cartesian 3N |
2 |
1 |
3 |
1 |
3 |
4 |
14 |
Translation (x,y,z) |
0 |
0 |
0 |
0 |
1 |
1 |
2 |
Rotation (Rx,Ry,Rz) |
0 |
1 |
1 |
0 |
0 |
0 |
2 |
Vibration |
2 |
0 |
2 |
1 |
2 |
3 |
10 |
Molecule Parameter
Number of Atoms (N) |
7 |
Number of internal coordinates |
15 |
Number of independant internal coordinates |
2 |
Number of vibrational modes |
10 |
Force field analysis
Allowed / forbidden vibronational transitions
Operator |
A1g |
A2g |
Eg |
A1u |
A2u |
Eu |
Total |
Linear (IR) |
2 |
0 |
2 |
1 |
2 |
3 |
5 / 5 |
Quadratic (Raman) |
2 |
0 |
2 |
1 |
2 |
3 |
4 / 6 |
IR + Raman |
- |
0 |
- |
1 |
- |
- |
0* / 1 |
* Center of inversion: Mutual Exclusion Principle
Characters of symmetric powers for vibration representation
Force field |
Tensor Order |
E |
2C3 |
3C'2 |
i |
2S6 |
3d |
linear |
1 |
15 |
0 |
1 |
-3 |
0 |
3 |
quadratic |
2 |
120 |
0 |
8 |
12 |
0 |
12 |
cubic |
3 |
680 |
5 |
8 |
-28 |
-1 |
28 |
quartic |
4 |
3.060 |
0 |
36 |
72 |
0 |
72 |
quintic |
5 |
11.628 |
0 |
36 |
-144 |
0 |
144 |
sextic |
6 |
38.760 |
15 |
120 |
300 |
3 |
300 |
Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field |
Tensor Order |
A1g |
A2g |
Eg |
A1u |
A2u |
Eu |
linear |
1 |
2 |
0 |
2 |
1 |
2 |
3 |
quadratic |
2 |
16 |
6 |
22 |
8 |
10 |
18 |
cubic |
3 |
64 |
46 |
108 |
55 |
65 |
117 |
quartic |
4 |
288 |
234 |
522 |
240 |
258 |
498 |
quintic |
5 |
1.002 |
912 |
1.914 |
954 |
1.008 |
1.962 |
sextic |
6 |
3.363 |
3.153 |
6.507 |
3.162 |
3.252 |
6.408 |
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