Characters of representations for molecular motions
Motion |
E |
C3 |
(C3)2 |
Cartesian 3N |
39 |
0 |
0 |
Translation (x,y,z) |
3 |
0 |
0 |
Rotation (Rx,Ry,Rz) |
3 |
0 |
0 |
Vibration |
33 |
0 |
0 |
Decomposition to irreducible representations
Motion |
A |
E*
|
Total |
Cartesian 3N |
13 |
13 |
26 |
Translation (x,y,z) |
1 |
1 |
2 |
Rotation (Rx,Ry,Rz) |
1 |
1 |
2 |
Vibration |
11 |
11 |
22 |
Molecular parameter
Number of Atoms (N) |
13
|
Number of internal coordinates |
33
|
Number of independant internal coordinates |
11
|
Number of vibrational modes |
22
|
Force field analysis
Allowed / forbidden vibronational transitions
Operator |
A |
E*
|
Total |
Linear (IR) |
11 |
11 |
22 / 0 |
Quadratic (Raman) |
11 |
11 |
22 / 0 |
IR + Raman |
11 |
11 |
22 / 0 |
Characters of force fields
(Symmetric powers of vibration representation)
Force field |
E |
C3 |
(C3)2 |
linear |
33 |
0 |
0 |
quadratic |
561 |
0 |
0 |
cubic |
6.545 |
11 |
11 |
quartic |
58.905 |
0 |
0 |
quintic |
435.897 |
0 |
0 |
sextic |
2.760.681 |
66 |
66 |
Decomposition to irreducible representations
Column with number of nonvanshing force constants highlighted
Force field |
A |
E*
|
linear |
11 |
11 |
quadratic |
187 |
187 |
cubic |
2.189 |
2.178 |
quartic |
19.635 |
19.635 |
quintic |
145.299 |
145.299 |
sextic |
920.271 |
920.205 |
Further Reading
- 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
- F. Varga, L. Nemes, J.K.G. Watson. J. Phys. B: At. Mol. Opt. Phys. 10 No. 7, 5043-5048 (1996)
The number of anharmonic potential constants of the fullerenes C60 and C70
Contributions to nonvanishing force field constants
pos(X) : Position of irreducible representation (irrep) X in character table of C
3
Subtotal: <Number of nonvanishing force constants in subsection> / <number of nonzero irrep combinations in subsection> / <number of irrep combinations in subsection>
Total: <Number of nonvanishing force constants in force field> / <number of nonzero irrep combinations in force field> / <number of irrep combinations in force field>
Contributions to nonvanishing quadratic force field constants
Irrep combinations (i,i) with indices: pos(A) ≤ i ≤ pos(E) |
..66. |
AA. | ..121. |
EE. | | |
| |
| |
| |
| |
| |
| |
| |
Subtotal: 187 / 2 / 2 |
Irrep combinations (i,j) with indices: pos(A) ≤ i ≤ j ≤ pos(E) |
Subtotal: 0 / 0 / 1 |
Total: 187 / 2 / 3 |
Contributions to nonvanishing cubic force field constants
Irrep combinations (i,i,i) with indices: pos(A) ≤ i ≤ pos(E) |
..286. |
AAA. | ..572. |
EEE. | | |
| |
| |
| |
| |
| |
| |
| |
Subtotal: 858 / 2 / 2 |
Irrep combinations (i,i,j) (i,j,j) with indices: pos(A) ≤ i ≤ j ≤ pos(E) |
..1.331. |
AEE. | | |
| |
| |
| |
| |
| |
| |
| |
| |
Subtotal: 1.331 / 1 / 2 |
Irrep combinations (i,j,k) with indices: pos(A) ≤ i ≤ j ≤ k ≤ pos(E) |
Subtotal: 0 / 0 / 0 |
Total: 2.189 / 3 / 4 |
Contributions to nonvanishing quartic force field constants
Irrep combinations (i,i,i,i) with indices: pos(A) ≤ i ≤ pos(E) |
..1.001. |
AAAA. | ..4.356. |
EEEE. | | |
| |
| |
| |
| |
| |
| |
| |
Subtotal: 5.357 / 2 / 2 |
Irrep combinations (i,i,i,j) (i,j,j,j) with indices: pos(A) ≤ i ≤ j ≤ pos(E) |
..6.292. |
AEEE. | | |
| |
| |
| |
| |
| |
| |
| |
| |
Subtotal: 6.292 / 1 / 2 |
Irrep combinations (i,i,j,j) with indices: pos(A) ≤ i ≤ j ≤ pos(E) |
..7.986. |
AAEE. | | |
| |
| |
| |
| |
| |
| |
| |
| |
Subtotal: 7.986 / 1 / 1 |
Irrep combinations (i,i,j,k) (i,j,j,k) (i,j,k,k) with indices: pos(A) ≤ i ≤ j ≤ k ≤ pos(E) |
Subtotal: 0 / 0 / 0 |
Irrep combinations (i,j,k,l) with indices: pos(A) ≤ i ≤ j ≤ k ≤ l ≤ pos(E) |
Subtotal: 0 / 0 / 0 |
Total: 19.635 / 4 / 5 |
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Last update November, 13th 2023 by A. Gelessus, Impressum, Datenschutzerklärung/DataPrivacyStatement