Characters of representations for molecular motions
Motion |
E |
2S8 |
2C4 |
2(S8)3 |
C2 |
4C'2 |
4σd |
Cartesian 3N |
24 |
0.000 |
0 |
-0.000 |
0 |
0 |
2 |
Translation (x,y,z) |
3 |
0.414 |
1 |
-2.414 |
-1 |
-1 |
1 |
Rotation (Rx,Ry,Rz) |
3 |
-0.414 |
1 |
2.414 |
-1 |
-1 |
-1 |
Vibration |
18 |
0.000 |
-2 |
0.000 |
2 |
2 |
2 |
Decomposition to irreducible representations
Motion |
A1 |
A2 |
B1 |
B2 |
E1 |
E2 |
E3 |
Total |
Cartesian 3N |
2 |
1 |
1 |
2 |
3 |
3 |
3 |
15 |
Translation (x,y,z) |
0 |
0 |
0 |
1 |
1 |
0 |
0 |
2 |
Rotation (Rx,Ry,Rz) |
0 |
1 |
0 |
0 |
0 |
0 |
1 |
2 |
Vibration |
2 |
0 |
1 |
1 |
2 |
3 |
2 |
11 |
Molecular parameter
Number of Atoms (N) |
8
|
Number of internal coordinates |
18
|
Number of independant internal coordinates |
2
|
Number of vibrational modes |
11
|
Force field analysis
Allowed / forbidden vibronational transitions
Operator |
A1 |
A2 |
B1 |
B2 |
E1 |
E2 |
E3 |
Total |
Linear (IR) |
2 |
0 |
1 |
1 |
2 |
3 |
2 |
3 / 8 |
Quadratic (Raman) |
2 |
0 |
1 |
1 |
2 |
3 |
2 |
7 / 4 |
IR + Raman |
- - - - |
0 |
1 |
- - - - |
- - - - |
- - - - |
- - - - |
0 / 1 |
Characters of force fields
(Symmetric powers of vibration representation)
Force field |
E |
2S8 |
2C4 |
2(S8)3 |
C2 |
4C'2 |
4σd |
linear |
18 |
0.000 |
-2 |
0.000 |
2 |
2 |
2 |
quadratic |
171 |
-1.000 |
3 |
-1.000 |
11 |
11 |
11 |
cubic |
1.140 |
-0.000 |
-4 |
-0.000 |
20 |
20 |
20 |
quartic |
5.985 |
1.000 |
9 |
1.000 |
65 |
65 |
65 |
quintic |
26.334 |
0.000 |
-14 |
0.000 |
110 |
110 |
110 |
sextic |
100.947 |
-1.000 |
19 |
-1.000 |
275 |
275 |
275 |
Decomposition to irreducible representations
Column with number of nonvanshing force constants highlighted
Force field |
A1 |
A2 |
B1 |
B2 |
E1 |
E2 |
E3 |
linear |
2 |
0 |
1 |
1 |
2 |
3 |
2 |
quadratic |
17 |
6 |
12 |
12 |
20 |
22 |
20 |
cubic |
82 |
62 |
72 |
72 |
140 |
146 |
140 |
quartic |
412 |
347 |
379 |
379 |
740 |
754 |
740 |
quintic |
1.706 |
1.596 |
1.651 |
1.651 |
3.278 |
3.309 |
3.278 |
sextic |
6.466 |
6.191 |
6.329 |
6.329 |
12.584 |
12.648 |
12.584 |
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
4d
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(A1) ≤ i ≤ pos(E3) |
..3. |
A1A1. | ..1. |
B1B1. | ..1. |
B2B2. | ..3. |
E1E1. | ..6. |
E2E2. | ..3. |
E3E3. | | |
| |
| |
| |
Subtotal: 17 / 6 / 7 |
Irrep combinations (i,j) with indices: pos(A1) ≤ i ≤ j ≤ pos(E3) |
Subtotal: 0 / 0 / 21 |
Total: 17 / 6 / 28 |
Contributions to nonvanishing cubic force field constants
Irrep combinations (i,i,i) with indices: pos(A1) ≤ i ≤ pos(E3) |
..4. |
A1A1A1. | | |
| |
| |
| |
| |
| |
| |
| |
| |
Subtotal: 4 / 1 / 7 |
Irrep combinations (i,i,j) (i,j,j) with indices: pos(A1) ≤ i ≤ j ≤ pos(E3) |
..9. |
E1E1E2. | ..2. |
A1B1B1. | ..2. |
A1B2B2. | ..6. |
A1E1E1. | ..12. |
A1E2E2. | ..6. |
A1E3E3. | ..6. |
B1E2E2. | ..6. |
B2E2E2. | ..9. |
E2E3E3. | | |
Subtotal: 58 / 9 / 42 |
Irrep combinations (i,j,k) with indices: pos(A1) ≤ i ≤ j ≤ k ≤ pos(E3) |
..4. |
B1E1E3. | ..4. |
B2E1E3. | ..12. |
E1E2E3. | | |
| |
| |
| |
| |
| |
| |
Subtotal: 20 / 3 / 35 |
Total: 82 / 13 / 84 |
Contributions to nonvanishing quartic force field constants
Irrep combinations (i,i,i,i) with indices: pos(A1) ≤ i ≤ pos(E3) |
..5. |
A1A1A1A1. | ..1. |
B1B1B1B1. | ..1. |
B2B2B2B2. | ..6. |
E1E1E1E1. | ..36. |
E2E2E2E2. | ..6. |
E3E3E3E3. | | |
| |
| |
| |
Subtotal: 55 / 6 / 7 |
Irrep combinations (i,i,i,j) (i,j,j,j) with indices: pos(A1) ≤ i ≤ j ≤ pos(E3) |
..8. |
E1E1E1E3. | ..8. |
E1E3E3E3. | | |
| |
| |
| |
| |
| |
| |
| |
Subtotal: 16 / 2 / 42 |
Irrep combinations (i,i,j,j) with indices: pos(A1) ≤ i ≤ j ≤ pos(E3) |
..3. |
A1A1B1B1. | ..3. |
A1A1B2B2. | ..9. |
A1A1E1E1. | ..18. |
A1A1E2E2. | ..9. |
A1A1E3E3. | ..1. |
B1B1B2B2. | ..3. |
B1B1E1E1. | ..6. |
B1B1E2E2. | ..3. |
B1B1E3E3. | ..3. |
B2B2E1E1. |
..6. |
B2B2E2E2. | ..3. |
B2B2E3E3. | ..21. |
E1E1E2E2. | ..19. |
E1E1E3E3. | ..21. |
E2E2E3E3. | | |
| |
| |
| |
| |
Subtotal: 128 / 15 / 21 |
Irrep combinations (i,i,j,k) (i,j,j,k) (i,j,k,k) with indices: pos(A1) ≤ i ≤ j ≤ k ≤ pos(E3) |
..18. |
A1E1E1E2. | ..9. |
B1E1E1E2. | ..9. |
B2E1E1E2. | ..48. |
E1E2E2E3. | ..12. |
A1B1E2E2. | ..12. |
A1B2E2E2. | ..18. |
A1E2E3E3. | ..1. |
B1B2E1E1. | ..3. |
B1B2E2E2. | ..1. |
B1B2E3E3. |
..9. |
B1E2E3E3. | ..9. |
B2E2E3E3. | | |
| |
| |
| |
| |
| |
| |
| |
Subtotal: 149 / 12 / 105 |
Irrep combinations (i,j,k,l) with indices: pos(A1) ≤ i ≤ j ≤ k ≤ l ≤ pos(E3) |
..8. |
A1B1E1E3. | ..8. |
A1B2E1E3. | ..24. |
A1E1E2E3. | ..12. |
B1E1E2E3. | ..12. |
B2E1E2E3. | | |
| |
| |
| |
| |
Subtotal: 64 / 5 / 35 |
Total: 412 / 40 / 210 |
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