Reduction formula for point group D4h
Characters for molecular motions
Motion |
E |
2C4 (z) |
C2 |
2C'2 |
2C''2 |
i |
2S4 |
h |
2v |
2d |
Cartesian 3N |
39 |
5 |
-5 |
-5 |
-1 |
-3 |
-1 |
9 |
9 |
5 |
Translation (x,y,z) |
3 |
1 |
-1 |
-1 |
-1 |
-3 |
-1 |
1 |
1 |
1 |
Rotation (Rx,Ry,Rz) |
3 |
1 |
-1 |
-1 |
-1 |
3 |
1 |
-1 |
-1 |
-1 |
Vibration |
33 |
3 |
-3 |
-3 |
1 |
-3 |
-1 |
9 |
9 |
5 |
Decomposition into Irreducible representations
Motion |
A1g |
A2g |
B1g |
B2g |
Eg |
A1u |
A2u |
B1u |
B2u |
Eu |
Total |
Cartesian 3N |
4 |
2 |
2 |
2 |
4 |
0 |
5 |
0 |
2 |
7 |
28 |
Translation (x,y,z) |
0 |
0 |
0 |
0 |
0 |
0 |
1 |
0 |
0 |
1 |
2 |
Rotation (Rx,Ry,Rz) |
0 |
1 |
0 |
0 |
1 |
0 |
0 |
0 |
0 |
0 |
2 |
Vibration |
4 |
1 |
2 |
2 |
3 |
0 |
4 |
0 |
2 |
6 |
24 |
Molecule Parameter
Number of Atoms (N) |
13 |
Number of internal coordinates |
33 |
Number of independant internal coordinates |
4 |
Number of vibrational modes |
24 |
Force field analysis
Allowed / forbidden vibronational transitions
Operator |
A1g |
A2g |
B1g |
B2g |
Eg |
A1u |
A2u |
B1u |
B2u |
Eu |
Total |
Linear (IR) |
4 |
1 |
2 |
2 |
3 |
0 |
4 |
0 |
2 |
6 |
10 / 14 |
Quadratic (Raman) |
4 |
1 |
2 |
2 |
3 |
0 |
4 |
0 |
2 |
6 |
11 / 13 |
IR + Raman |
- |
1 |
- |
- |
- |
0 |
- |
0 |
2 |
- |
0* / 3 |
* Center of inversion: Mutual Exclusion Principle
Characters of symmetric powers for vibration representation
Force field |
Tensor Order |
E |
2C4 (z) |
C2 |
2C'2 |
2C''2 |
i |
2S4 |
h |
2v |
2d |
linear |
1 |
33 |
3 |
-3 |
-3 |
1 |
-3 |
-1 |
9 |
9 |
5 |
quadratic |
2 |
561 |
3 |
21 |
21 |
17 |
21 |
-1 |
57 |
57 |
29 |
cubic |
3 |
6.545 |
1 |
-55 |
-55 |
17 |
-55 |
1 |
273 |
273 |
105 |
quartic |
4 |
58.905 |
9 |
225 |
225 |
153 |
225 |
9 |
1.113 |
1.113 |
385 |
quintic |
5 |
435.897 |
27 |
-531 |
-531 |
153 |
-531 |
-9 |
3.969 |
3.969 |
1.141 |
sextic |
6 |
2.760.681 |
27 |
1.653 |
1.653 |
969 |
1.653 |
-9 |
12.817 |
12.817 |
3.325 |
Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field |
Tensor Order |
A1g |
A2g |
B1g |
B2g |
Eg |
A1u |
A2u |
B1u |
B2u |
Eu |
linear |
1 |
4 |
1 |
2 |
2 |
3 |
0 |
4 |
0 |
2 |
6 |
quadratic |
2 |
57 |
26 |
45 |
37 |
63 |
26 |
38 |
28 |
34 |
72 |
cubic |
3 |
462 |
377 |
431 |
407 |
784 |
340 |
444 |
362 |
422 |
866 |
quartic |
4 |
4.016 |
3.547 |
3.877 |
3.677 |
7.224 |
3.472 |
3.752 |
3.530 |
3.694 |
7.446 |
quintic |
5 |
28.019 |
26.836 |
27.691 |
27.155 |
53.991 |
26.314 |
27.686 |
26.552 |
27.430 |
55.116 |
sextic |
6 |
175.898 |
171.207 |
174.820 |
172.276 |
343.483 |
170.056 |
173.436 |
170.636 |
172.838 |
346.274 |
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