Reduction formula for point group D3
Characters for molecular motions
Motion |
E |
2C3 (z) |
3C'2 |
Cartesian 3N |
120 |
0 |
0 |
Translation (x,y,z) |
3 |
0 |
-1 |
Rotation (Rx,Ry,Rz) |
3 |
0 |
-1 |
Vibration |
114 |
0 |
2 |
Decomposition into Irreducible representations
Motion |
A1 |
A2 |
E |
Total |
Cartesian 3N |
20 |
20 |
40 |
80 |
Translation (x,y,z) |
0 |
1 |
1 |
2 |
Rotation (Rx,Ry,Rz) |
0 |
1 |
1 |
2 |
Vibration |
20 |
18 |
38 |
76 |
Molecule Parameter
Number of Atoms (N) |
40 |
Number of internal coordinates |
114 |
Number of independant internal coordinates |
20 |
Number of vibrational modes |
76 |
Force field analysis
Allowed / forbidden vibronational transitions
Operator |
A1 |
A2 |
E |
Total |
Linear (IR) |
20 |
18 |
38 |
56 / 20 |
Quadratic (Raman) |
20 |
18 |
38 |
58 / 18 |
IR + Raman |
- |
- |
38 |
38 / 0 |
Characters of symmetric powers for vibration representation
Force field |
Tensor Order |
E |
2C3 (z) |
3C'2 |
linear |
1 |
114 |
0 |
2 |
quadratic |
2 |
6.555 |
0 |
59 |
cubic |
3 |
253.460 |
38 |
116 |
quartic |
4 |
7.413.705 |
0 |
1.769 |
quintic |
5 |
174.963.438 |
0 |
3.422 |
sextic |
6 |
3.470.108.187 |
741 |
35.931 |
Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field |
Tensor Order |
A1 |
A2 |
E |
linear |
1 |
20 |
18 |
38 |
quadratic |
2 |
1.122 |
1.063 |
2.185 |
cubic |
3 |
42.314 |
42.198 |
84.474 |
quartic |
4 |
1.236.502 |
1.234.733 |
2.471.235 |
quintic |
5 |
29.162.284 |
29.158.862 |
58.321.146 |
sextic |
6 |
578.369.577 |
578.333.646 |
1.156.702.482 |
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