Reduction formula for point group D2d
Characters for molecular motions
Motion |
E |
2S4 |
C2 (z) |
2C'2 |
2d |
Cartesian 3N |
36 |
0 |
-4 |
0 |
8 |
Translation (x,y,z) |
3 |
-1 |
-1 |
-1 |
1 |
Rotation (Rx,Ry,Rz) |
3 |
1 |
-1 |
-1 |
-1 |
Vibration |
30 |
0 |
-2 |
2 |
8 |
Decomposition into Irreducible representations
Motion |
A1 |
A2 |
B1 |
B2 |
E |
Total |
Cartesian 3N |
6 |
2 |
2 |
6 |
10 |
26 |
Translation (x,y,z) |
0 |
0 |
0 |
1 |
1 |
2 |
Rotation (Rx,Ry,Rz) |
0 |
1 |
0 |
0 |
1 |
2 |
Vibration |
6 |
1 |
2 |
5 |
8 |
22 |
Molecule Parameter
Number of Atoms (N) |
12 |
Number of internal coordinates |
30 |
Number of independant internal coordinates |
6 |
Number of vibrational modes |
22 |
Force field analysis
Allowed / forbidden vibronational transitions
Operator |
A1 |
A2 |
B1 |
B2 |
E |
Total |
Linear (IR) |
6 |
1 |
2 |
5 |
8 |
13 / 9 |
Quadratic (Raman) |
6 |
1 |
2 |
5 |
8 |
21 / 1 |
IR + Raman |
- |
1 |
- |
5 |
8 |
13 / 1 |
Characters of symmetric powers for vibration representation
Force field |
Tensor Order |
E |
2S4 |
C2 (z) |
2C'2 |
2d |
linear |
1 |
30 |
0 |
-2 |
2 |
8 |
quadratic |
2 |
465 |
-1 |
17 |
17 |
47 |
cubic |
3 |
4.960 |
0 |
-32 |
32 |
208 |
quartic |
4 |
40.920 |
8 |
152 |
152 |
792 |
quintic |
5 |
278.256 |
0 |
-272 |
272 |
2.640 |
sextic |
6 |
1.623.160 |
-8 |
952 |
952 |
8.008 |
Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field |
Tensor Order |
A1 |
A2 |
B1 |
B2 |
E |
linear |
1 |
6 |
1 |
2 |
5 |
8 |
quadratic |
2 |
76 |
44 |
53 |
68 |
112 |
cubic |
3 |
676 |
556 |
572 |
660 |
1.248 |
quartic |
4 |
5.372 |
4.900 |
4.972 |
5.292 |
10.192 |
quintic |
5 |
35.476 |
34.020 |
34.156 |
35.340 |
69.632 |
sextic |
6 |
205.252 |
200.772 |
201.252 |
204.780 |
405.552 |
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