Characters of representations for molecular motions
Motion |
E |
2S12 |
2C6 |
2S4 |
2C3 |
2(S12)5 |
C2 |
6C'2 |
6σd |
Cartesian 3N |
75 |
0.732 |
2 |
-1 |
0 |
-2.732 |
-1 |
-1 |
5 |
Translation (x,y,z) |
3 |
0.732 |
2 |
-1 |
0 |
-2.732 |
-1 |
-1 |
1 |
Rotation (Rx,Ry,Rz) |
3 |
-0.732 |
2 |
1 |
0 |
2.732 |
-1 |
-1 |
-1 |
Vibration |
69 |
0.732 |
-2 |
-1 |
0 |
-2.732 |
1 |
1 |
5 |
Decomposition to irreducible representations
Motion |
A1 |
A2 |
B1 |
B2 |
E1 |
E2 |
E3 |
E4 |
E5 |
Total |
Cartesian 3N |
4 |
2 |
2 |
5 |
7 |
6 |
6 |
6 |
6 |
44 |
Translation (x,y,z) |
0 |
0 |
0 |
1 |
1 |
0 |
0 |
0 |
0 |
2 |
Rotation (Rx,Ry,Rz) |
0 |
1 |
0 |
0 |
0 |
0 |
0 |
0 |
1 |
2 |
Vibration |
4 |
1 |
2 |
4 |
6 |
6 |
6 |
6 |
5 |
40 |
Molecular parameter
Number of Atoms (N) |
25
|
Number of internal coordinates |
69
|
Number of independant internal coordinates |
4
|
Number of vibrational modes |
40
|
Force field analysis
Allowed / forbidden vibronational transitions
Operator |
A1 |
A2 |
B1 |
B2 |
E1 |
E2 |
E3 |
E4 |
E5 |
Total |
Linear (IR) |
4 |
1 |
2 |
4 |
6 |
6 |
6 |
6 |
5 |
10 / 30 |
Quadratic (Raman) |
4 |
1 |
2 |
4 |
6 |
6 |
6 |
6 |
5 |
15 / 25 |
IR + Raman |
- - - - |
1 |
2 |
- - - - |
- - - - |
- - - - |
6 |
6 |
- - - - |
0 / 15 |
Characters of force fields
(Symmetric powers of vibration representation)
Force field |
E |
2S12 |
2C6 |
2S4 |
2C3 |
2(S12)5 |
C2 |
6C'2 |
6σd |
linear |
69 |
0.732 |
-2 |
-1 |
0 |
-2.732 |
1 |
1 |
5 |
quadratic |
2.415 |
-0.732 |
2 |
1 |
0 |
2.732 |
35 |
35 |
47 |
cubic |
57.155 |
-1.000 |
-1 |
-1 |
23 |
-1.000 |
35 |
35 |
195 |
quartic |
1.028.790 |
0.000 |
0 |
18 |
0 |
0.000 |
630 |
630 |
1.078 |
quintic |
15.020.334 |
-0.000 |
0 |
-18 |
0 |
-0.000 |
630 |
630 |
3.886 |
sextic |
185.250.786 |
-0.000 |
12 |
18 |
276 |
0.000 |
7.770 |
7.770 |
16.354 |
Decomposition to irreducible representations
Column with number of nonvanshing force constants highlighted
Force field |
A1 |
A2 |
B1 |
B2 |
E1 |
E2 |
E3 |
E4 |
E5 |
linear |
4 |
1 |
2 |
4 |
6 |
6 |
6 |
6 |
5 |
quadratic |
123 |
82 |
99 |
105 |
198 |
204 |
198 |
204 |
199 |
cubic |
2.442 |
2.327 |
2.345 |
2.425 |
4.758 |
4.764 |
4.764 |
4.764 |
4.758 |
quartic |
43.321 |
42.467 |
42.779 |
43.003 |
85.680 |
85.782 |
85.680 |
85.788 |
85.680 |
quintic |
627.001 |
624.743 |
625.061 |
626.689 |
1.251.642 |
1.251.750 |
1.251.642 |
1.251.744 |
1.251.642 |
sextic |
7.725.163 |
7.713.101 |
7.716.983 |
7.721.275 |
15.436.896 |
15.438.186 |
15.436.962 |
15.438.192 |
15.436.896 |
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
6d
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(E5) |
..10. |
A1A1. | ..1. |
A2A2. | ..3. |
B1B1. | ..10. |
B2B2. | ..21. |
E1E1. | ..21. |
E2E2. | ..21. |
E3E3. | ..21. |
E4E4. | ..15. |
E5E5. | | |
Subtotal: 123 / 9 / 9 |
Irrep combinations (i,j) with indices: pos(A1) ≤ i ≤ j ≤ pos(E5) |
Subtotal: 0 / 0 / 36 |
Total: 123 / 9 / 45 |
Contributions to nonvanishing cubic force field constants
Irrep combinations (i,i,i) with indices: pos(A1) ≤ i ≤ pos(E5) |
..20. |
A1A1A1. | ..56. |
E4E4E4. | | |
| |
| |
| |
| |
| |
| |
| |
Subtotal: 76 / 2 / 9 |
Irrep combinations (i,i,j) (i,j,j) with indices: pos(A1) ≤ i ≤ j ≤ pos(E5) |
..126. |
E1E1E2. | ..126. |
E2E2E4. | ..4. |
A1A2A2. | ..12. |
A1B1B1. | ..40. |
A1B2B2. | ..84. |
A1E1E1. | ..84. |
A1E2E2. | ..84. |
A1E3E3. | ..84. |
A1E4E4. | ..60. |
A1E5E5. |
..15. |
A2E1E1. | ..15. |
A2E2E2. | ..15. |
A2E3E3. | ..15. |
A2E4E4. | ..10. |
A2E5E5. | ..42. |
B1E3E3. | ..84. |
B2E3E3. | ..90. |
E2E5E5. | | |
| |
Subtotal: 990 / 18 / 72 |
Irrep combinations (i,j,k) with indices: pos(A1) ≤ i ≤ j ≤ k ≤ pos(E5) |
..8. |
A2B1B2. | ..60. |
B1E1E5. | ..72. |
B1E2E4. | ..120. |
B2E1E5. | ..144. |
B2E2E4. | ..216. |
E1E2E3. | ..216. |
E1E3E4. | ..180. |
E1E4E5. | ..180. |
E2E3E5. | ..180. |
E3E4E5. |
Subtotal: 1.376 / 10 / 84 |
Total: 2.442 / 30 / 165 |
Contributions to nonvanishing quartic force field constants
Irrep combinations (i,i,i,i) with indices: pos(A1) ≤ i ≤ pos(E5) |
..35. |
A1A1A1A1. | ..1. |
A2A2A2A2. | ..5. |
B1B1B1B1. | ..35. |
B2B2B2B2. | ..231. |
E1E1E1E1. | ..231. |
E2E2E2E2. | ..357. |
E3E3E3E3. | ..231. |
E4E4E4E4. | ..120. |
E5E5E5E5. | | |
Subtotal: 1.246 / 9 / 9 |
Irrep combinations (i,i,i,j) (i,j,j,j) with indices: pos(A1) ≤ i ≤ j ≤ pos(E5) |
..336. |
E1E1E1E3. | ..224. |
A1E4E4E4. | ..56. |
A2E4E4E4. | ..112. |
B1E2E2E2. | ..224. |
B2E2E2E2. | ..210. |
E3E5E5E5. | | |
| |
| |
| |
Subtotal: 1.162 / 6 / 72 |
Irrep combinations (i,i,j,j) with indices: pos(A1) ≤ i ≤ j ≤ pos(E5) |
..10. |
A1A1A2A2. | ..30. |
A1A1B1B1. | ..100. |
A1A1B2B2. | ..210. |
A1A1E1E1. | ..210. |
A1A1E2E2. | ..210. |
A1A1E3E3. | ..210. |
A1A1E4E4. | ..150. |
A1A1E5E5. | ..3. |
A2A2B1B1. | ..10. |
A2A2B2B2. |
..21. |
A2A2E1E1. | ..21. |
A2A2E2E2. | ..21. |
A2A2E3E3. | ..21. |
A2A2E4E4. | ..15. |
A2A2E5E5. | ..30. |
B1B1B2B2. | ..63. |
B1B1E1E1. | ..63. |
B1B1E2E2. | ..63. |
B1B1E3E3. | ..63. |
B1B1E4E4. |
..45. |
B1B1E5E5. | ..210. |
B2B2E1E1. | ..210. |
B2B2E2E2. | ..210. |
B2B2E3E3. | ..210. |
B2B2E4E4. | ..150. |
B2B2E5E5. | ..666. |
E1E1E2E2. | ..666. |
E1E1E3E3. | ..666. |
E1E1E4E4. | ..780. |
E1E1E5E5. |
..666. |
E2E2E3E3. | ..1.107. |
E2E2E4E4. | ..465. |
E2E2E5E5. | ..666. |
E3E3E4E4. | ..465. |
E3E3E5E5. | ..465. |
E4E4E5E5. | | |
| |
| |
| |
Subtotal: 9.171 / 36 / 36 |
Irrep combinations (i,i,j,k) (i,j,j,k) (i,j,k,k) with indices: pos(A1) ≤ i ≤ j ≤ k ≤ pos(E5) |
..756. |
E1E1E2E4. | ..630. |
E1E1E3E5. | ..630. |
E2E2E3E5. | ..504. |
A1E1E1E2. | ..504. |
A1E2E2E4. | ..126. |
A2E1E1E2. | ..126. |
A2E2E2E4. | ..252. |
B1E1E1E4. | ..504. |
B2E1E1E4. | ..756. |
E1E2E2E3. |
..630. |
E1E2E2E5. | ..1.260. |
E1E3E3E5. | ..630. |
E1E4E4E5. | ..1.512. |
E2E3E3E4. | ..630. |
E3E4E4E5. | ..60. |
A1A2E1E1. | ..60. |
A1A2E2E2. | ..60. |
A1A2E3E3. | ..60. |
A1A2E4E4. | ..40. |
A1A2E5E5. |
..168. |
A1B1E3E3. | ..336. |
A1B2E3E3. | ..360. |
A1E2E5E5. | ..42. |
A2B1E3E3. | ..84. |
A2B2E3E3. | ..90. |
A2E2E5E5. | ..120. |
B1B2E1E1. | ..120. |
B1B2E2E2. | ..120. |
B1B2E3E3. | ..120. |
B1B2E4E4. |
..80. |
B1B2E5E5. | ..252. |
B1E2E4E4. | ..180. |
B1E4E5E5. | ..504. |
B2E2E4E4. | ..360. |
B2E4E5E5. | ..756. |
E1E3E4E4. | ..540. |
E1E3E5E5. | ..540. |
E2E4E5E5. | | |
| |
Subtotal: 14.502 / 38 / 252 |
Irrep combinations (i,j,k,l) with indices: pos(A1) ≤ i ≤ j ≤ k ≤ l ≤ pos(E5) |
..32. |
A1A2B1B2. | ..240. |
A1B1E1E5. | ..288. |
A1B1E2E4. | ..480. |
A1B2E1E5. | ..576. |
A1B2E2E4. | ..864. |
A1E1E2E3. | ..864. |
A1E1E3E4. | ..720. |
A1E1E4E5. | ..720. |
A1E2E3E5. | ..720. |
A1E3E4E5. |
..60. |
A2B1E1E5. | ..72. |
A2B1E2E4. | ..120. |
A2B2E1E5. | ..144. |
A2B2E2E4. | ..216. |
A2E1E2E3. | ..216. |
A2E1E3E4. | ..180. |
A2E1E4E5. | ..180. |
A2E2E3E5. | ..180. |
A2E3E4E5. | ..432. |
B1E1E2E3. |
..360. |
B1E1E2E5. | ..432. |
B1E1E3E4. | ..360. |
B1E2E3E5. | ..360. |
B1E3E4E5. | ..864. |
B2E1E2E3. | ..720. |
B2E1E2E5. | ..864. |
B2E1E3E4. | ..720. |
B2E2E3E5. | ..720. |
B2E3E4E5. | ..1.296. |
E1E2E3E4. |
..2.160. |
E1E2E4E5. | ..1.080. |
E2E3E4E5. | | |
| |
| |
| |
| |
| |
| |
| |
Subtotal: 17.240 / 32 / 126 |
Total: 43.321 / 121 / 495 |
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Last update November, 13th 2023 by A. Gelessus, Impressum, Datenschutzerklärung/DataPrivacyStatement