Reduction formula for point group C6v
Characters for molecular motions
Motion |
E |
2C6 (z) |
2C3 (z) |
C2 (z) |
3v |
3d |
Cartesian 3N |
15 |
10 |
0 |
-5 |
5 |
5 |
Translation (x,y,z) |
3 |
2 |
0 |
-1 |
1 |
1 |
Rotation (Rx,Ry)* |
2 |
1 |
-1 |
-2 |
0 |
0 |
Vibration |
10 |
7 |
1 |
-2 |
4 |
4 |
* Linear molecule
Decomposition into Irreducible representations
Motion |
A1 |
A2 |
B1 |
B2 |
E1 |
E2 |
Total |
Cartesian 3N |
5 |
0 |
0 |
0 |
5 |
0 |
10 |
Translation (x,y,z) |
1 |
0 |
0 |
0 |
1 |
0 |
2 |
Rotation (Rx,Ry)* |
0 |
0 |
0 |
0 |
1 |
0 |
1 |
Vibration |
4 |
0 |
0 |
0 |
3 |
0 |
7 |
* Linear molecule
Molecule Parameter
Number of Atoms (N) |
5 |
Number of internal coordinates |
10 |
Number of independant internal coordinates |
4 |
Number of vibrational modes |
7 |
Force field analysis
Allowed / forbidden vibronational transitions
Operator |
A1 |
A2 |
B1 |
B2 |
E1 |
E2 |
Total |
Linear (IR) |
4 |
0 |
0 |
0 |
3 |
0 |
7 / 0 |
Quadratic (Raman) |
4 |
0 |
0 |
0 |
3 |
0 |
7 / 0 |
IR + Raman |
4 |
0 |
0 |
0 |
3 |
- |
7 / 0 |
Characters of symmetric powers for vibration representation
Force field |
Tensor Order |
E |
2C6 (z) |
2C3 (z) |
C2 (z) |
3v |
3d |
linear |
1 |
10 |
7 |
1 |
-2 |
4 |
4 |
quadratic |
2 |
55 |
25 |
1 |
7 |
13 |
13 |
cubic |
3 |
220 |
60 |
4 |
-12 |
32 |
32 |
quartic |
4 |
715 |
108 |
4 |
27 |
71 |
71 |
quintic |
5 |
2.002 |
156 |
4 |
-42 |
140 |
140 |
sextic |
6 |
5.005 |
194 |
10 |
77 |
259 |
259 |
Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field |
Tensor Order |
A1 |
A2 |
B1 |
B2 |
E1 |
E2 |
linear |
1 |
4 |
0 |
0 |
0 |
3 |
0 |
quadratic |
2 |
16 |
3 |
0 |
0 |
12 |
6 |
cubic |
3 |
44 |
12 |
10 |
10 |
48 |
24 |
quartic |
4 |
116 |
45 |
40 |
40 |
132 |
105 |
quintic |
5 |
260 |
120 |
145 |
145 |
366 |
300 |
sextic |
6 |
587 |
328 |
380 |
380 |
852 |
813 |
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