Reduction formula for point group D2d
Characters for molecular motions
Motion |
E |
2S4 |
C2 (z) |
2C'2 |
2d |
Cartesian 3N |
48 |
0 |
0 |
-4 |
4 |
Translation (x,y,z) |
3 |
-1 |
-1 |
-1 |
1 |
Rotation (Rx,Ry,Rz) |
3 |
1 |
-1 |
-1 |
-1 |
Vibration |
42 |
0 |
2 |
-2 |
4 |
Decomposition into Irreducible representations
Motion |
A1 |
A2 |
B1 |
B2 |
E |
Total |
Cartesian 3N |
6 |
6 |
4 |
8 |
12 |
36 |
Translation (x,y,z) |
0 |
0 |
0 |
1 |
1 |
2 |
Rotation (Rx,Ry,Rz) |
0 |
1 |
0 |
0 |
1 |
2 |
Vibration |
6 |
5 |
4 |
7 |
10 |
32 |
Molecule Parameter
Number of Atoms (N) |
16 |
Number of internal coordinates |
42 |
Number of independant internal coordinates |
6 |
Number of vibrational modes |
32 |
Force field analysis
Allowed / forbidden vibronational transitions
Operator |
A1 |
A2 |
B1 |
B2 |
E |
Total |
Linear (IR) |
6 |
5 |
4 |
7 |
10 |
17 / 15 |
Quadratic (Raman) |
6 |
5 |
4 |
7 |
10 |
27 / 5 |
IR + Raman |
- |
5 |
- |
7 |
10 |
17 / 5 |
Characters of symmetric powers for vibration representation
Force field |
Tensor Order |
E |
2S4 |
C2 (z) |
2C'2 |
2d |
linear |
1 |
42 |
0 |
2 |
-2 |
4 |
quadratic |
2 |
903 |
1 |
23 |
23 |
29 |
cubic |
3 |
13.244 |
0 |
44 |
-44 |
96 |
quartic |
4 |
148.995 |
11 |
275 |
275 |
415 |
quintic |
5 |
1.370.754 |
0 |
506 |
-506 |
1.196 |
sextic |
6 |
10.737.573 |
11 |
2.277 |
2.277 |
3.979 |
Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field |
Tensor Order |
A1 |
A2 |
B1 |
B2 |
E |
linear |
1 |
6 |
5 |
4 |
7 |
10 |
quadratic |
2 |
129 |
103 |
114 |
117 |
220 |
cubic |
3 |
1.674 |
1.648 |
1.626 |
1.696 |
3.300 |
quartic |
4 |
18.834 |
18.489 |
18.621 |
18.691 |
37.180 |
quintic |
5 |
171.580 |
171.235 |
170.982 |
171.833 |
342.562 |
sextic |
6 |
1.344.048 |
1.340.920 |
1.342.053 |
1.342.904 |
2.683.824 |
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