Reduction formula for point group D6h
Characters for molecular motions
Motion |
E |
2C6 (z) |
2C3 |
C2 |
3C'2 |
3C''2 |
i |
2S3 |
2S6 |
h (xy) |
3d |
3v |
Cartesian 3N |
75 |
2 |
0 |
-1 |
-1 |
-1 |
-3 |
-2 |
0 |
1 |
1 |
9 |
Translation (x,y,z) |
3 |
2 |
0 |
-1 |
-1 |
-1 |
-3 |
-2 |
0 |
1 |
1 |
1 |
Rotation (Rx,Ry,Rz) |
3 |
2 |
0 |
-1 |
-1 |
-1 |
3 |
2 |
0 |
-1 |
-1 |
-1 |
Vibration |
69 |
-2 |
0 |
1 |
1 |
1 |
-3 |
-2 |
0 |
1 |
1 |
9 |
Decomposition into Irreducible representations
Motion |
A1g |
A2g |
B1g |
B2g |
E1g |
E2g |
A1u |
A2u |
B1u |
B2u |
E1u |
E2u |
Total |
Cartesian 3N |
4 |
2 |
2 |
4 |
6 |
6 |
2 |
5 |
4 |
2 |
7 |
6 |
50 |
Translation (x,y,z) |
0 |
0 |
0 |
0 |
0 |
0 |
0 |
1 |
0 |
0 |
1 |
0 |
2 |
Rotation (Rx,Ry,Rz) |
0 |
1 |
0 |
0 |
1 |
0 |
0 |
0 |
0 |
0 |
0 |
0 |
2 |
Vibration |
4 |
1 |
2 |
4 |
5 |
6 |
2 |
4 |
4 |
2 |
6 |
6 |
46 |
Molecule Parameter
Number of Atoms (N) |
25 |
Number of internal coordinates |
69 |
Number of independant internal coordinates |
4 |
Number of vibrational modes |
46 |
Force field analysis
Allowed / forbidden vibronational transitions
Operator |
A1g |
A2g |
B1g |
B2g |
E1g |
E2g |
A1u |
A2u |
B1u |
B2u |
E1u |
E2u |
Total |
Linear (IR) |
4 |
1 |
2 |
4 |
5 |
6 |
2 |
4 |
4 |
2 |
6 |
6 |
10 / 36 |
Quadratic (Raman) |
4 |
1 |
2 |
4 |
5 |
6 |
2 |
4 |
4 |
2 |
6 |
6 |
15 / 31 |
IR + Raman |
- |
1 |
2 |
4 |
- |
- |
2 |
- |
4 |
2 |
- |
6 |
0* / 21 |
* Center of inversion: Mutual Exclusion Principle
Characters of symmetric powers for vibration representation
Force field |
Tensor Order |
E |
2C6 (z) |
2C3 |
C2 |
3C'2 |
3C''2 |
i |
2S3 |
2S6 |
h (xy) |
3d |
3v |
linear |
1 |
69 |
-2 |
0 |
1 |
1 |
1 |
-3 |
-2 |
0 |
1 |
1 |
9 |
quadratic |
2 |
2.415 |
2 |
0 |
35 |
35 |
35 |
39 |
2 |
0 |
35 |
35 |
75 |
cubic |
3 |
57.155 |
-1 |
23 |
35 |
35 |
35 |
-109 |
-1 |
-1 |
35 |
35 |
435 |
quartic |
4 |
1.028.790 |
0 |
0 |
630 |
630 |
630 |
774 |
0 |
0 |
630 |
630 |
2.310 |
quintic |
5 |
15.020.334 |
0 |
0 |
630 |
630 |
630 |
-2.034 |
0 |
0 |
630 |
630 |
10.422 |
sextic |
6 |
185.250.786 |
12 |
276 |
7.770 |
7.770 |
7.770 |
10.434 |
12 |
12 |
7.770 |
7.770 |
43.738 |
Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field |
Tensor Order |
A1g |
A2g |
B1g |
B2g |
E1g |
E2g |
A1u |
A2u |
B1u |
B2u |
E1u |
E2u |
linear |
1 |
4 |
1 |
2 |
4 |
5 |
6 |
2 |
4 |
4 |
2 |
6 |
6 |
quadratic |
2 |
128 |
83 |
94 |
104 |
199 |
210 |
94 |
104 |
104 |
94 |
198 |
198 |
cubic |
3 |
2.449 |
2.314 |
2.326 |
2.426 |
4.746 |
4.758 |
2.338 |
2.438 |
2.438 |
2.338 |
4.770 |
4.770 |
quartic |
4 |
43.476 |
42.426 |
42.636 |
43.056 |
85.692 |
85.902 |
42.624 |
43.044 |
43.044 |
42.624 |
85.668 |
85.668 |
quintic |
5 |
627.354 |
624.276 |
624.486 |
626.934 |
1.251.420 |
1.251.630 |
624.708 |
627.156 |
627.156 |
624.708 |
1.251.864 |
1.251.864 |
sextic |
6 |
7.728.272 |
7.711.510 |
7.714.096 |
7.723.088 |
15.437.118 |
15.439.704 |
7.713.874 |
7.722.866 |
7.722.866 |
7.713.874 |
15.436.674 |
15.436.674 |
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