Characters of representations for molecular motions
Motion |
E |
2C5 |
2(C5)2 |
5C'2 |
i |
2(S10)3 |
2S10 |
5σd |
Cartesian 3N |
63 |
1.618 |
-0.618 |
-1 |
-3 |
-1.618 |
0.618 |
5 |
Translation (x,y,z) |
3 |
1.618 |
-0.618 |
-1 |
-3 |
-1.618 |
0.618 |
1 |
Rotation (Rx,Ry,Rz) |
3 |
1.618 |
-0.618 |
-1 |
3 |
1.618 |
-0.618 |
-1 |
Vibration |
57 |
-1.618 |
0.618 |
1 |
-3 |
-1.618 |
0.618 |
5 |
Decomposition to irreducible representations
Motion |
A1g |
A2g |
E1g |
E2g |
A1u |
A2u |
E1u |
E2u |
Total |
Cartesian 3N |
4 |
2 |
6 |
6 |
2 |
5 |
7 |
6 |
38 |
Translation (x,y,z) |
0 |
0 |
0 |
0 |
0 |
1 |
1 |
0 |
2 |
Rotation (Rx,Ry,Rz) |
0 |
1 |
1 |
0 |
0 |
0 |
0 |
0 |
2 |
Vibration |
4 |
1 |
5 |
6 |
2 |
4 |
6 |
6 |
34 |
Molecular parameter
Number of Atoms (N) |
21
|
Number of internal coordinates |
57
|
Number of independant internal coordinates |
4
|
Number of vibrational modes |
34
|
Force field analysis
Allowed / forbidden vibronational transitions
Operator |
A1g |
A2g |
E1g |
E2g |
A1u |
A2u |
E1u |
E2u |
Total |
Linear (IR) |
4 |
1 |
5 |
6 |
2 |
4 |
6 |
6 |
10 / 24 |
Quadratic (Raman) |
4 |
1 |
5 |
6 |
2 |
4 |
6 |
6 |
15 / 19 |
IR + Raman |
- - - - |
1 |
- - - - |
- - - - |
2 |
- - - - |
- - - - |
6 |
0* / 9 |
* Parity Mutual Exclusion Principle
Characters of force fields
(Symmetric powers of vibration representation)
Force field |
E |
2C5 |
2(C5)2 |
5C'2 |
i |
2(S10)3 |
2S10 |
5σd |
linear |
57 |
-1.618 |
0.618 |
1 |
-3 |
-1.618 |
0.618 |
5 |
quadratic |
1.653 |
1.618 |
-0.618 |
29 |
33 |
1.618 |
-0.618 |
41 |
cubic |
32.509 |
-1.000 |
-1.000 |
29 |
-91 |
-1.000 |
-1.000 |
165 |
quartic |
487.635 |
-0.000 |
0.000 |
435 |
555 |
-0.000 |
-0.000 |
811 |
quintic |
5.949.147 |
12.000 |
12.000 |
435 |
-1.425 |
-0.000 |
-0.000 |
2.791 |
sextic |
61.474.519 |
-19.416 |
7.416 |
4.495 |
6.355 |
0.000 |
0.000 |
10.571 |
Decomposition to irreducible representations
Column with number of nonvanshing force constants highlighted
Force field |
A1g |
A2g |
E1g |
E2g |
A1u |
A2u |
E1u |
E2u |
linear |
4 |
1 |
5 |
6 |
2 |
4 |
6 |
6 |
quadratic |
102 |
67 |
169 |
168 |
78 |
84 |
162 |
162 |
cubic |
1.669 |
1.572 |
3.242 |
3.242 |
1.596 |
1.664 |
3.260 |
3.260 |
quartic |
24.721 |
24.098 |
48.819 |
48.819 |
24.260 |
24.448 |
48.708 |
48.708 |
quintic |
298.195 |
296.582 |
594.771 |
594.771 |
296.942 |
298.120 |
595.056 |
595.056 |
sextic |
3.077.809 |
3.070.276 |
6.148.085 |
6.148.091 |
3.071.888 |
3.074.926 |
6.146.814 |
6.146.820 |
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
5d
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(E2u) |
..10. |
A1gA1g. | ..1. |
A2gA2g. | ..15. |
E1gE1g. | ..21. |
E2gE2g. | ..3. |
A1uA1u. | ..10. |
A2uA2u. | ..21. |
E1uE1u. | ..21. |
E2uE2u. | | |
| |
Subtotal: 102 / 8 / 8 |
Irrep combinations (i,j) with indices: pos(A1g) ≤ i ≤ j ≤ pos(E2u) |
Subtotal: 0 / 0 / 28 |
Total: 102 / 8 / 36 |
Contributions to nonvanishing cubic force field constants
Irrep combinations (i,i,i) with indices: pos(A1g) ≤ i ≤ pos(E2u) |
..20. |
A1gA1gA1g. | | |
| |
| |
| |
| |
| |
| |
| |
| |
Subtotal: 20 / 1 / 8 |
Irrep combinations (i,i,j) (i,j,j) with indices: pos(A1g) ≤ i ≤ j ≤ pos(E2u) |
..90. |
E1gE1gE2g. | ..4. |
A1gA2gA2g. | ..60. |
A1gE1gE1g. | ..84. |
A1gE2gE2g. | ..12. |
A1gA1uA1u. | ..40. |
A1gA2uA2u. | ..84. |
A1gE1uE1u. | ..84. |
A1gE2uE2u. | ..10. |
A2gE1gE1g. | ..15. |
A2gE2gE2g. |
..15. |
A2gE1uE1u. | ..15. |
A2gE2uE2u. | ..105. |
E1gE2gE2g. | ..105. |
E1gE2uE2u. | ..126. |
E2gE1uE1u. | | |
| |
| |
| |
| |
Subtotal: 849 / 15 / 56 |
Irrep combinations (i,j,k) with indices: pos(A1g) ≤ i ≤ j ≤ k ≤ pos(E2u) |
..8. |
A2gA1uA2u. | ..60. |
E1gA1uE1u. | ..120. |
E1gA2uE1u. | ..180. |
E1gE1uE2u. | ..72. |
E2gA1uE2u. | ..144. |
E2gA2uE2u. | ..216. |
E2gE1uE2u. | | |
| |
| |
Subtotal: 800 / 7 / 56 |
Total: 1.669 / 23 / 120 |
Contributions to nonvanishing quartic force field constants
Irrep combinations (i,i,i,i) with indices: pos(A1g) ≤ i ≤ pos(E2u) |
..35. |
A1gA1gA1gA1g. | ..1. |
A2gA2gA2gA2g. | ..120. |
E1gE1gE1gE1g. | ..231. |
E2gE2gE2gE2g. | ..5. |
A1uA1uA1uA1u. | ..35. |
A2uA2uA2uA2u. | ..231. |
E1uE1uE1uE1u. | ..231. |
E2uE2uE2uE2u. | | |
| |
Subtotal: 889 / 8 / 8 |
Irrep combinations (i,i,i,j) (i,j,j,j) with indices: pos(A1g) ≤ i ≤ j ≤ pos(E2u) |
..210. |
E1gE1gE1gE2g. | ..336. |
E1uE1uE1uE2u. | ..280. |
E1gE2gE2gE2g. | ..336. |
E1uE2uE2uE2u. | | |
| |
| |
| |
| |
| |
Subtotal: 1.162 / 4 / 56 |
Irrep combinations (i,i,j,j) with indices: pos(A1g) ≤ i ≤ j ≤ pos(E2u) |
..10. |
A1gA1gA2gA2g. | ..150. |
A1gA1gE1gE1g. | ..210. |
A1gA1gE2gE2g. | ..30. |
A1gA1gA1uA1u. | ..100. |
A1gA1gA2uA2u. | ..210. |
A1gA1gE1uE1u. | ..210. |
A1gA1gE2uE2u. | ..15. |
A2gA2gE1gE1g. | ..21. |
A2gA2gE2gE2g. | ..3. |
A2gA2gA1uA1u. |
..10. |
A2gA2gA2uA2u. | ..21. |
A2gA2gE1uE1u. | ..21. |
A2gA2gE2uE2u. | ..465. |
E1gE1gE2gE2g. | ..45. |
E1gE1gA1uA1u. | ..150. |
E1gE1gA2uA2u. | ..780. |
E1gE1gE1uE1u. | ..465. |
E1gE1gE2uE2u. | ..63. |
E2gE2gA1uA1u. | ..210. |
E2gE2gA2uA2u. |
..666. |
E2gE2gE1uE1u. | ..1.107. |
E2gE2gE2uE2u. | ..30. |
A1uA1uA2uA2u. | ..63. |
A1uA1uE1uE1u. | ..63. |
A1uA1uE2uE2u. | ..210. |
A2uA2uE1uE1u. | ..210. |
A2uA2uE2uE2u. | ..666. |
E1uE1uE2uE2u. | | |
| |
Subtotal: 6.204 / 28 / 28 |
Irrep combinations (i,i,j,k) (i,j,j,k) (i,j,k,k) with indices: pos(A1g) ≤ i ≤ j ≤ k ≤ pos(E2u) |
..80. |
E1gE1gA1uA2u. | ..180. |
E1gE1gA1uE2u. | ..360. |
E1gE1gA2uE2u. | ..540. |
E1gE1gE1uE2u. | ..120. |
E2gE2gA1uA2u. | ..252. |
E2gE2gA1uE1u. | ..504. |
E2gE2gA2uE1u. | ..756. |
E2gE2gE1uE2u. | ..360. |
A1gE1gE1gE2g. | ..90. |
A2gE1gE1gE2g. |
..252. |
A1uE1uE1uE2u. | ..504. |
A2uE1uE1uE2u. | ..40. |
A1gA2gE1gE1g. | ..60. |
A1gA2gE2gE2g. | ..60. |
A1gA2gE1uE1u. | ..60. |
A1gA2gE2uE2u. | ..420. |
A1gE1gE2gE2g. | ..420. |
A1gE1gE2uE2u. | ..504. |
A1gE2gE1uE1u. | ..105. |
A2gE1gE2gE2g. |
..105. |
A2gE1gE2uE2u. | ..126. |
A2gE2gE1uE1u. | ..630. |
E1gE2gE1uE1u. | ..630. |
E1gE2gE2uE2u. | ..120. |
A1uA2uE1uE1u. | ..120. |
A1uA2uE2uE2u. | ..252. |
A1uE1uE2uE2u. | ..504. |
A2uE1uE2uE2u. | | |
| |
Subtotal: 8.154 / 28 / 168 |
Irrep combinations (i,j,k,l) with indices: pos(A1g) ≤ i ≤ j ≤ k ≤ l ≤ pos(E2u) |
..32. |
A1gA2gA1uA2u. | ..240. |
A1gE1gA1uE1u. | ..480. |
A1gE1gA2uE1u. | ..720. |
A1gE1gE1uE2u. | ..288. |
A1gE2gA1uE2u. | ..576. |
A1gE2gA2uE2u. | ..864. |
A1gE2gE1uE2u. | ..60. |
A2gE1gA1uE1u. | ..120. |
A2gE1gA2uE1u. | ..180. |
A2gE1gE1uE2u. |
..72. |
A2gE2gA1uE2u. | ..144. |
A2gE2gA2uE2u. | ..216. |
A2gE2gE1uE2u. | ..360. |
E1gE2gA1uE1u. | ..360. |
E1gE2gA1uE2u. | ..720. |
E1gE2gA2uE1u. | ..720. |
E1gE2gA2uE2u. | ..2.160. |
E1gE2gE1uE2u. | | |
| |
Subtotal: 8.312 / 18 / 70 |
Total: 24.721 / 86 / 330 |
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Last update November, 13th 2023 by A. Gelessus, Impressum, Datenschutzerklärung/DataPrivacyStatement