Reduction formula for point group D2d
Characters for molecular motions
Motion |
E |
2S4 |
C2 (z) |
2C'2 |
2d |
Cartesian 3N |
39 |
-1 |
-5 |
-1 |
9 |
Translation (x,y,z) |
3 |
-1 |
-1 |
-1 |
1 |
Rotation (Rx,Ry,Rz) |
3 |
1 |
-1 |
-1 |
-1 |
Vibration |
33 |
-1 |
-3 |
1 |
9 |
Decomposition into Irreducible representations
Motion |
A1 |
A2 |
B1 |
B2 |
E |
Total |
Cartesian 3N |
6 |
2 |
2 |
7 |
11 |
28 |
Translation (x,y,z) |
0 |
0 |
0 |
1 |
1 |
2 |
Rotation (Rx,Ry,Rz) |
0 |
1 |
0 |
0 |
1 |
2 |
Vibration |
6 |
1 |
2 |
6 |
9 |
24 |
Molecule Parameter
Number of Atoms (N) |
13 |
Number of internal coordinates |
33 |
Number of independant internal coordinates |
6 |
Number of vibrational modes |
24 |
Force field analysis
Allowed / forbidden vibronational transitions
Operator |
A1 |
A2 |
B1 |
B2 |
E |
Total |
Linear (IR) |
6 |
1 |
2 |
6 |
9 |
15 / 9 |
Quadratic (Raman) |
6 |
1 |
2 |
6 |
9 |
23 / 1 |
IR + Raman |
- |
1 |
- |
6 |
9 |
15 / 1 |
Characters of symmetric powers for vibration representation
Force field |
Tensor Order |
E |
2S4 |
C2 (z) |
2C'2 |
2d |
linear |
1 |
33 |
-1 |
-3 |
1 |
9 |
quadratic |
2 |
561 |
-1 |
21 |
17 |
57 |
cubic |
3 |
6.545 |
1 |
-55 |
17 |
273 |
quartic |
4 |
58.905 |
9 |
225 |
153 |
1.113 |
quintic |
5 |
435.897 |
-9 |
-531 |
153 |
3.969 |
sextic |
6 |
2.760.681 |
-9 |
1.653 |
969 |
12.817 |
Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field |
Tensor Order |
A1 |
A2 |
B1 |
B2 |
E |
linear |
1 |
6 |
1 |
2 |
6 |
9 |
quadratic |
2 |
91 |
54 |
63 |
83 |
135 |
cubic |
3 |
884 |
739 |
747 |
875 |
1.650 |
quartic |
4 |
7.710 |
7.077 |
7.149 |
7.629 |
14.670 |
quintic |
5 |
55.449 |
53.388 |
53.469 |
55.377 |
109.107 |
sextic |
6 |
348.736 |
341.843 |
342.332 |
348.256 |
689.757 |
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