Reduction formula for point group D2
Characters for molecular motions
Motion |
E |
C2 (z) |
C2 (y) |
C2 (x) |
Cartesian 3N |
15 |
-5 |
-1 |
-1 |
Translation (x,y,z) |
3 |
-1 |
-1 |
-1 |
Rotation (Rx,Ry)* |
2 |
-2 |
0 |
0 |
Vibration |
10 |
-2 |
0 |
0 |
* Linear molecule
Decomposition into Irreducible representations
Motion |
A |
B1 |
B2 |
B3 |
Total |
Cartesian 3N |
2 |
3 |
5 |
5 |
15 |
Translation (x,y,z) |
0 |
1 |
1 |
1 |
3 |
Rotation (Rx,Ry)* |
0 |
0 |
1 |
1 |
2 |
Vibration |
2 |
2 |
3 |
3 |
10 |
* Linear molecule
Molecule Parameter
Number of Atoms (N) |
5 |
Number of internal coordinates |
10 |
Number of independant internal coordinates |
2 |
Number of vibrational modes |
10 |
Force field analysis
Allowed / forbidden vibronational transitions
Operator |
A |
B1 |
B2 |
B3 |
Total |
Linear (IR) |
2 |
2 |
3 |
3 |
8 / 2 |
Quadratic (Raman) |
2 |
2 |
3 |
3 |
10 / 0 |
IR + Raman |
- |
2 |
3 |
3 |
8 / 0 |
Characters of symmetric powers for vibration representation
Force field |
Tensor Order |
E |
C2 (z) |
C2 (y) |
C2 (x) |
linear |
1 |
10 |
-2 |
0 |
0 |
quadratic |
2 |
55 |
7 |
5 |
5 |
cubic |
3 |
220 |
-12 |
0 |
0 |
quartic |
4 |
715 |
27 |
15 |
15 |
quintic |
5 |
2.002 |
-42 |
0 |
0 |
sextic |
6 |
5.005 |
77 |
35 |
35 |
Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field |
Tensor Order |
A |
B1 |
B2 |
B3 |
linear |
1 |
2 |
2 |
3 |
3 |
quadratic |
2 |
18 |
13 |
12 |
12 |
cubic |
3 |
52 |
52 |
58 |
58 |
quartic |
4 |
193 |
178 |
172 |
172 |
quintic |
5 |
490 |
490 |
511 |
511 |
sextic |
6 |
1.288 |
1.253 |
1.232 |
1.232 |
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