Reduction formula for point group D2
Characters for molecular motions
Motion |
E |
C2 (z) |
C2 (y) |
C2 (x) |
Cartesian 3N |
252 |
0 |
0 |
0 |
Translation (x,y,z) |
3 |
-1 |
-1 |
-1 |
Rotation (Rx,Ry,Rz) |
3 |
-1 |
-1 |
-1 |
Vibration |
246 |
2 |
2 |
2 |
Decomposition into Irreducible representations
Motion |
A |
B1 |
B2 |
B3 |
Total |
Cartesian 3N |
63 |
63 |
63 |
63 |
252 |
Translation (x,y,z) |
0 |
1 |
1 |
1 |
3 |
Rotation (Rx,Ry,Rz) |
0 |
1 |
1 |
1 |
3 |
Vibration |
63 |
61 |
61 |
61 |
246 |
Molecule Parameter
Number of Atoms (N) |
84 |
Number of internal coordinates |
246 |
Number of independant internal coordinates |
63 |
Number of vibrational modes |
246 |
Force field analysis
Allowed / forbidden vibronational transitions
Operator |
A |
B1 |
B2 |
B3 |
Total |
Linear (IR) |
63 |
61 |
61 |
61 |
183 / 63 |
Quadratic (Raman) |
63 |
61 |
61 |
61 |
246 / 0 |
IR + Raman |
- |
61 |
61 |
61 |
183 / 0 |
Characters of symmetric powers for vibration representation
Force field |
Tensor Order |
E |
C2 (z) |
C2 (y) |
C2 (x) |
linear |
1 |
246 |
2 |
2 |
2 |
quadratic |
2 |
30.381 |
125 |
125 |
125 |
cubic |
3 |
2.511.496 |
248 |
248 |
248 |
quartic |
4 |
156.340.626 |
7.874 |
7.874 |
7.874 |
quintic |
5 |
7.817.031.300 |
15.500 |
15.500 |
15.500 |
sextic |
6 |
327.012.476.050 |
333.250 |
333.250 |
333.250 |
Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field |
Tensor Order |
A |
B1 |
B2 |
B3 |
linear |
1 |
63 |
61 |
61 |
61 |
quadratic |
2 |
7.689 |
7.564 |
7.564 |
7.564 |
cubic |
3 |
628.060 |
627.812 |
627.812 |
627.812 |
quartic |
4 |
39.091.062 |
39.083.188 |
39.083.188 |
39.083.188 |
quintic |
5 |
1.954.269.450 |
1.954.253.950 |
1.954.253.950 |
1.954.253.950 |
sextic |
6 |
81.753.368.950 |
81.753.035.700 |
81.753.035.700 |
81.753.035.700 |
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