Reduction formula for point group D4
Characters for molecular motions
Motion |
E |
2C4 (z) |
C2 (z) |
2C'2 |
2C''2 |
Cartesian 3N |
36 |
4 |
-4 |
-4 |
0 |
Translation (x,y,z) |
3 |
1 |
-1 |
-1 |
-1 |
Rotation (Rx,Ry,Rz) |
3 |
1 |
-1 |
-1 |
-1 |
Vibration |
30 |
2 |
-2 |
-2 |
2 |
Decomposition into Irreducible representations
Motion |
A1 |
A2 |
B1 |
B2 |
E |
Total |
Cartesian 3N |
4 |
6 |
2 |
4 |
10 |
26 |
Translation (x,y,z) |
0 |
1 |
0 |
0 |
1 |
2 |
Rotation (Rx,Ry,Rz) |
0 |
1 |
0 |
0 |
1 |
2 |
Vibration |
4 |
4 |
2 |
4 |
8 |
22 |
Molecule Parameter
Number of Atoms (N) |
12 |
Number of internal coordinates |
30 |
Number of independant internal coordinates |
4 |
Number of vibrational modes |
22 |
Force field analysis
Allowed / forbidden vibronational transitions
Operator |
A1 |
A2 |
B1 |
B2 |
E |
Total |
Linear (IR) |
4 |
4 |
2 |
4 |
8 |
12 / 10 |
Quadratic (Raman) |
4 |
4 |
2 |
4 |
8 |
18 / 4 |
IR + Raman |
- |
- |
- |
- |
8 |
8 / 0 |
Characters of symmetric powers for vibration representation
Force field |
Tensor Order |
E |
2C4 (z) |
C2 (z) |
2C'2 |
2C''2 |
linear |
1 |
30 |
2 |
-2 |
-2 |
2 |
quadratic |
2 |
465 |
1 |
17 |
17 |
17 |
cubic |
3 |
4.960 |
0 |
-32 |
-32 |
32 |
quartic |
4 |
40.920 |
8 |
152 |
152 |
152 |
quintic |
5 |
278.256 |
16 |
-272 |
-272 |
272 |
sextic |
6 |
1.623.160 |
8 |
952 |
952 |
952 |
Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field |
Tensor Order |
A1 |
A2 |
B1 |
B2 |
E |
linear |
1 |
4 |
4 |
2 |
4 |
8 |
quadratic |
2 |
69 |
52 |
60 |
60 |
112 |
cubic |
3 |
616 |
616 |
600 |
632 |
1.248 |
quartic |
4 |
5.212 |
5.060 |
5.132 |
5.132 |
10.192 |
quintic |
5 |
34.752 |
34.752 |
34.608 |
34.880 |
69.632 |
sextic |
6 |
203.492 |
202.540 |
203.012 |
203.012 |
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