Reduction formula for point group C2
Characters for molecular motions
| Motion |
E |
C2 |
| Cartesian 3N |
216 |
-8 |
| Translation (x,y,z) |
3 |
-1 |
| Rotation (Rx,Ry,Rz) |
3 |
-1 |
| Vibration |
210 |
-6 |
Decomposition into Irreducible representations
| Motion |
A |
B |
Total |
| Cartesian 3N |
104 |
112 |
216 |
| Translation (x,y,z) |
1 |
2 |
3 |
| Rotation (Rx,Ry,Rz) |
1 |
2 |
3 |
| Vibration |
102 |
108 |
210 |
Molecule Parameter
| Number of Atoms (N) |
72 |
| Number of internal coordinates |
210 |
| Number of independant internal coordinates |
102 |
| Number of vibrational modes |
210 |
Force field analysis
Allowed / forbidden vibronational transitions
| Operator |
A |
B |
Total |
| Linear (IR) |
102 |
108 |
210 / 0 |
| Quadratic (Raman) |
102 |
108 |
210 / 0 |
| IR + Raman |
102 |
108 |
210 / 0 |
Characters of symmetric powers for vibration representation
| Force field |
Tensor
Order |
E |
C2 |
| linear |
1 |
210 |
-6 |
| quadratic |
2 |
22.155 |
123 |
| cubic |
3 |
1.565.620 |
-668 |
| quartic |
4 |
83.369.265 |
7.521 |
| quintic |
5 |
3.568.204.542 |
-37.482 |
| sextic |
6 |
127.860.662.755 |
305.731 |
Decomposition into Irreducible representations
Number of nonvanshing force constants
| Force field |
Tensor
Order |
A |
B |
| linear |
1 |
102 |
108 |
| quadratic |
2 |
11.139 |
11.016 |
| cubic |
3 |
782.476 |
783.144 |
| quartic |
4 |
41.688.393 |
41.680.872 |
| quintic |
5 |
1.784.083.530 |
1.784.121.012 |
| sextic |
6 |
63.930.484.243 |
63.930.178.512 |
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