Characters of representations for molecular motions
Motion |
E |
2C3 |
3C'2 |
σh |
2S3 |
3σv |
Cartesian 3N |
27 |
0 |
-1 |
3 |
0 |
3 |
Translation (x,y,z) |
3 |
0 |
-1 |
1 |
-2 |
1 |
Rotation (Rx,Ry,Rz) |
3 |
0 |
-1 |
-1 |
2 |
-1 |
Vibration |
21 |
0 |
1 |
3 |
0 |
3 |
Decomposition to irreducible representations
Motion |
A'1 |
A'2 |
E' |
A''1 |
A''2 |
E'' |
Total |
Cartesian 3N |
3 |
2 |
5 |
1 |
3 |
4 |
18 |
Translation (x,y,z) |
0 |
0 |
1 |
0 |
1 |
0 |
2 |
Rotation (Rx,Ry,Rz) |
0 |
1 |
0 |
0 |
0 |
1 |
2 |
Vibration |
3 |
1 |
4 |
1 |
2 |
3 |
14 |
Molecular parameter
Number of Atoms (N) |
9
|
Number of internal coordinates |
21
|
Number of independant internal coordinates |
3
|
Number of vibrational modes |
14
|
Force field analysis
Allowed / forbidden vibronational transitions
Operator |
A'1 |
A'2 |
E' |
A''1 |
A''2 |
E'' |
Total |
Linear (IR) |
3 |
1 |
4 |
1 |
2 |
3 |
6 / 8 |
Quadratic (Raman) |
3 |
1 |
4 |
1 |
2 |
3 |
10 / 4 |
IR + Raman |
- - - - |
1 |
4 |
1 |
- - - - |
- - - - |
4 / 2 |
Characters of force fields
(Symmetric powers of vibration representation)
Force field |
E |
2C3 |
3C'2 |
σh |
2S3 |
3σv |
linear |
21 |
0 |
1 |
3 |
0 |
3 |
quadratic |
231 |
0 |
11 |
15 |
0 |
15 |
cubic |
1.771 |
7 |
11 |
37 |
1 |
37 |
quartic |
10.626 |
0 |
66 |
114 |
0 |
114 |
quintic |
53.130 |
0 |
66 |
246 |
0 |
246 |
sextic |
230.230 |
28 |
286 |
598 |
4 |
598 |
Decomposition to irreducible representations
Column with number of nonvanshing force constants highlighted
Force field |
A'1 |
A'2 |
E' |
A''1 |
A''2 |
E'' |
linear |
3 |
1 |
4 |
1 |
2 |
3 |
quadratic |
27 |
14 |
41 |
17 |
19 |
36 |
cubic |
164 |
140 |
300 |
139 |
152 |
288 |
quartic |
940 |
850 |
1.790 |
864 |
888 |
1.752 |
quintic |
4.526 |
4.370 |
8.896 |
4.362 |
4.452 |
8.814 |
sextic |
19.462 |
19.020 |
38.466 |
19.062 |
19.218 |
38.268 |
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 D
3h
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'1) ≤ i ≤ pos(E'') |
..6. |
A'1A'1. | ..1. |
A'2A'2. | ..10. |
E'E'. | ..1. |
A''1A''1. | ..3. |
A''2A''2. | ..6. |
E''E''. | | |
| |
| |
| |
Subtotal: 27 / 6 / 6 |
Irrep combinations (i,j) with indices: pos(A'1) ≤ i ≤ j ≤ pos(E'') |
Subtotal: 0 / 0 / 15 |
Total: 27 / 6 / 21 |
Contributions to nonvanishing cubic force field constants
Irrep combinations (i,i,i) with indices: pos(A'1) ≤ i ≤ pos(E'') |
..10. |
A'1A'1A'1. | ..20. |
E'E'E'. | | |
| |
| |
| |
| |
| |
| |
| |
Subtotal: 30 / 2 / 6 |
Irrep combinations (i,i,j) (i,j,j) with indices: pos(A'1) ≤ i ≤ j ≤ pos(E'') |
..3. |
A'1A'2A'2. | ..30. |
A'1E'E'. | ..3. |
A'1A''1A''1. | ..9. |
A'1A''2A''2. | ..18. |
A'1E''E''. | ..6. |
A'2E'E'. | ..3. |
A'2E''E''. | ..24. |
E'E''E''. | | |
| |
Subtotal: 96 / 8 / 30 |
Irrep combinations (i,j,k) with indices: pos(A'1) ≤ i ≤ j ≤ k ≤ pos(E'') |
..2. |
A'2A''1A''2. | ..12. |
E'A''1E''. | ..24. |
E'A''2E''. | | |
| |
| |
| |
| |
| |
| |
Subtotal: 38 / 3 / 20 |
Total: 164 / 13 / 56 |
Contributions to nonvanishing quartic force field constants
Irrep combinations (i,i,i,i) with indices: pos(A'1) ≤ i ≤ pos(E'') |
..15. |
A'1A'1A'1A'1. | ..1. |
A'2A'2A'2A'2. | ..55. |
E'E'E'E'. | ..1. |
A''1A''1A''1A''1. | ..5. |
A''2A''2A''2A''2. | ..21. |
E''E''E''E''. | | |
| |
| |
| |
Subtotal: 98 / 6 / 6 |
Irrep combinations (i,i,i,j) (i,j,j,j) with indices: pos(A'1) ≤ i ≤ j ≤ pos(E'') |
..60. |
A'1E'E'E'. | ..20. |
A'2E'E'E'. | ..10. |
A''1E''E''E''. | ..20. |
A''2E''E''E''. | | |
| |
| |
| |
| |
| |
Subtotal: 110 / 4 / 30 |
Irrep combinations (i,i,j,j) with indices: pos(A'1) ≤ i ≤ j ≤ pos(E'') |
..6. |
A'1A'1A'2A'2. | ..60. |
A'1A'1E'E'. | ..6. |
A'1A'1A''1A''1. | ..18. |
A'1A'1A''2A''2. | ..36. |
A'1A'1E''E''. | ..10. |
A'2A'2E'E'. | ..1. |
A'2A'2A''1A''1. | ..3. |
A'2A'2A''2A''2. | ..6. |
A'2A'2E''E''. | ..10. |
E'E'A''1A''1. |
..30. |
E'E'A''2A''2. | ..138. |
E'E'E''E''. | ..3. |
A''1A''1A''2A''2. | ..6. |
A''1A''1E''E''. | ..18. |
A''2A''2E''E''. | | |
| |
| |
| |
| |
Subtotal: 351 / 15 / 15 |
Irrep combinations (i,i,j,k) (i,j,j,k) (i,j,k,k) with indices: pos(A'1) ≤ i ≤ j ≤ k ≤ pos(E'') |
..12. |
E'E'A''1A''2. | ..30. |
E'E'A''1E''. | ..60. |
E'E'A''2E''. | ..18. |
A'1A'2E'E'. | ..9. |
A'1A'2E''E''. | ..72. |
A'1E'E''E''. | ..24. |
A'2E'E''E''. | ..6. |
A''1A''2E''E''. | | |
| |
Subtotal: 231 / 8 / 60 |
Irrep combinations (i,j,k,l) with indices: pos(A'1) ≤ i ≤ j ≤ k ≤ l ≤ pos(E'') |
..6. |
A'1A'2A''1A''2. | ..36. |
A'1E'A''1E''. | ..72. |
A'1E'A''2E''. | ..12. |
A'2E'A''1E''. | ..24. |
A'2E'A''2E''. | | |
| |
| |
| |
| |
Subtotal: 150 / 5 / 15 |
Total: 940 / 38 / 126 |
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