Characters of representations for molecular motions
Motion |
E |
2C3 |
3C'2 |
i |
2S6 |
3σd |
Cartesian 3N |
36 |
0 |
0 |
0 |
0 |
4 |
Translation (x,y,z) |
3 |
0 |
-1 |
-3 |
0 |
1 |
Rotation (Rx,Ry,Rz) |
3 |
0 |
-1 |
3 |
0 |
-1 |
Vibration |
30 |
0 |
2 |
0 |
0 |
4 |
Decomposition to irreducible representations
Motion |
A1g |
A2g |
Eg |
A1u |
A2u |
Eu |
Total |
Cartesian 3N |
4 |
2 |
6 |
2 |
4 |
6 |
24 |
Translation (x,y,z) |
0 |
0 |
0 |
0 |
1 |
1 |
2 |
Rotation (Rx,Ry,Rz) |
0 |
1 |
1 |
0 |
0 |
0 |
2 |
Vibration |
4 |
1 |
5 |
2 |
3 |
5 |
20 |
Molecular parameter
Number of Atoms (N) |
12
|
Number of internal coordinates |
30
|
Number of independant internal coordinates |
4
|
Number of vibrational modes |
20
|
Force field analysis
Allowed / forbidden vibronational transitions
Operator |
A1g |
A2g |
Eg |
A1u |
A2u |
Eu |
Total |
Linear (IR) |
4 |
1 |
5 |
2 |
3 |
5 |
8 / 12 |
Quadratic (Raman) |
4 |
1 |
5 |
2 |
3 |
5 |
9 / 11 |
IR + Raman |
- - - - |
1 |
- - - - |
2 |
- - - - |
- - - - |
0* / 3 |
* Parity Mutual Exclusion Principle
Characters of force fields
(Symmetric powers of vibration representation)
Force field |
E |
2C3 |
3C'2 |
i |
2S6 |
3σd |
linear |
30 |
0 |
2 |
0 |
0 |
4 |
quadratic |
465 |
0 |
17 |
15 |
0 |
23 |
cubic |
4.960 |
10 |
32 |
0 |
0 |
72 |
quartic |
40.920 |
0 |
152 |
120 |
0 |
256 |
quintic |
278.256 |
0 |
272 |
0 |
0 |
680 |
sextic |
1.623.160 |
55 |
952 |
680 |
5 |
1.904 |
Decomposition to irreducible representations
Column with number of nonvanshing force constants highlighted
Force field |
A1g |
A2g |
Eg |
A1u |
A2u |
Eu |
linear |
4 |
1 |
5 |
2 |
3 |
5 |
quadratic |
50 |
30 |
80 |
36 |
39 |
75 |
cubic |
441 |
389 |
825 |
405 |
425 |
825 |
quartic |
3.522 |
3.318 |
6.840 |
3.374 |
3.426 |
6.800 |
quintic |
23.426 |
22.950 |
46.376 |
23.086 |
23.290 |
46.376 |
sextic |
136.044 |
134.616 |
270.630 |
134.977 |
135.453 |
270.405 |
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
3d
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(A1g) ≤ i ≤ pos(Eu) |
..10. |
A1gA1g. | ..1. |
A2gA2g. | ..15. |
EgEg. | ..3. |
A1uA1u. | ..6. |
A2uA2u. | ..15. |
EuEu. | | |
| |
| |
| |
Subtotal: 50 / 6 / 6 |
Irrep combinations (i,j) with indices: pos(A1g) ≤ i ≤ j ≤ pos(Eu) |
Subtotal: 0 / 0 / 15 |
Total: 50 / 6 / 21 |
Contributions to nonvanishing cubic force field constants
Irrep combinations (i,i,i) with indices: pos(A1g) ≤ i ≤ pos(Eu) |
..20. |
A1gA1gA1g. | ..35. |
EgEgEg. | | |
| |
| |
| |
| |
| |
| |
| |
Subtotal: 55 / 2 / 6 |
Irrep combinations (i,i,j) (i,j,j) with indices: pos(A1g) ≤ i ≤ j ≤ pos(Eu) |
..4. |
A1gA2gA2g. | ..60. |
A1gEgEg. | ..12. |
A1gA1uA1u. | ..24. |
A1gA2uA2u. | ..60. |
A1gEuEu. | ..10. |
A2gEgEg. | ..10. |
A2gEuEu. | ..75. |
EgEuEu. | | |
| |
Subtotal: 255 / 8 / 30 |
Irrep combinations (i,j,k) with indices: pos(A1g) ≤ i ≤ j ≤ k ≤ pos(Eu) |
..6. |
A2gA1uA2u. | ..50. |
EgA1uEu. | ..75. |
EgA2uEu. | | |
| |
| |
| |
| |
| |
| |
Subtotal: 131 / 3 / 20 |
Total: 441 / 13 / 56 |
Contributions to nonvanishing quartic force field constants
Irrep combinations (i,i,i,i) with indices: pos(A1g) ≤ i ≤ pos(Eu) |
..35. |
A1gA1gA1gA1g. | ..1. |
A2gA2gA2gA2g. | ..120. |
EgEgEgEg. | ..5. |
A1uA1uA1uA1u. | ..15. |
A2uA2uA2uA2u. | ..120. |
EuEuEuEu. | | |
| |
| |
| |
Subtotal: 296 / 6 / 6 |
Irrep combinations (i,i,i,j) (i,j,j,j) with indices: pos(A1g) ≤ i ≤ j ≤ pos(Eu) |
..140. |
A1gEgEgEg. | ..35. |
A2gEgEgEg. | ..70. |
A1uEuEuEu. | ..105. |
A2uEuEuEu. | | |
| |
| |
| |
| |
| |
Subtotal: 350 / 4 / 30 |
Irrep combinations (i,i,j,j) with indices: pos(A1g) ≤ i ≤ j ≤ pos(Eu) |
..10. |
A1gA1gA2gA2g. | ..150. |
A1gA1gEgEg. | ..30. |
A1gA1gA1uA1u. | ..60. |
A1gA1gA2uA2u. | ..150. |
A1gA1gEuEu. | ..15. |
A2gA2gEgEg. | ..3. |
A2gA2gA1uA1u. | ..6. |
A2gA2gA2uA2u. | ..15. |
A2gA2gEuEu. | ..45. |
EgEgA1uA1u. |
..90. |
EgEgA2uA2u. | ..550. |
EgEgEuEu. | ..18. |
A1uA1uA2uA2u. | ..45. |
A1uA1uEuEu. | ..90. |
A2uA2uEuEu. | | |
| |
| |
| |
| |
Subtotal: 1.277 / 15 / 15 |
Irrep combinations (i,i,j,k) (i,j,j,k) (i,j,k,k) with indices: pos(A1g) ≤ i ≤ j ≤ k ≤ pos(Eu) |
..60. |
EgEgA1uA2u. | ..150. |
EgEgA1uEu. | ..225. |
EgEgA2uEu. | ..40. |
A1gA2gEgEg. | ..40. |
A1gA2gEuEu. | ..300. |
A1gEgEuEu. | ..75. |
A2gEgEuEu. | ..60. |
A1uA2uEuEu. | | |
| |
Subtotal: 950 / 8 / 60 |
Irrep combinations (i,j,k,l) with indices: pos(A1g) ≤ i ≤ j ≤ k ≤ l ≤ pos(Eu) |
..24. |
A1gA2gA1uA2u. | ..200. |
A1gEgA1uEu. | ..300. |
A1gEgA2uEu. | ..50. |
A2gEgA1uEu. | ..75. |
A2gEgA2uEu. | | |
| |
| |
| |
| |
Subtotal: 649 / 5 / 15 |
Total: 3.522 / 38 / 126 |
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