Characters of representations for molecular motions
Motion |
E |
i |
Cartesian 3N |
36 |
0 |
Translation (x,y,z) |
3 |
-3 |
Rotation (Rx,Ry,Rz) |
3 |
3 |
Vibration |
30 |
0 |
Decomposition to irreducible representations
Motion |
Ag |
Au |
Total |
Cartesian 3N |
18 |
18 |
36 |
Translation (x,y,z) |
0 |
3 |
3 |
Rotation (Rx,Ry,Rz) |
3 |
0 |
3 |
Vibration |
15 |
15 |
30 |
Molecular parameter
Number of Atoms (N) |
12
|
Number of internal coordinates |
30
|
Number of independant internal coordinates |
15
|
Number of vibrational modes |
30
|
Force field analysis
Allowed / forbidden vibronational transitions
Operator |
Ag |
Au |
Total |
Linear (IR) |
15 |
15 |
15 / 15 |
Quadratic (Raman) |
15 |
15 |
15 / 15 |
IR + Raman |
- - - - |
- - - - |
0* / 0 |
* Parity Mutual Exclusion Principle
Characters of force fields
(Symmetric powers of vibration representation)
Force field |
E |
i |
linear |
30 |
0 |
quadratic |
465 |
15 |
cubic |
4.960 |
0 |
quartic |
40.920 |
120 |
quintic |
278.256 |
0 |
sextic |
1.623.160 |
680 |
Decomposition to irreducible representations
Column with number of nonvanshing force constants highlighted
Force field |
Ag |
Au |
linear |
15 |
15 |
quadratic |
240 |
225 |
cubic |
2.480 |
2.480 |
quartic |
20.520 |
20.400 |
quintic |
139.128 |
139.128 |
sextic |
811.920 |
811.240 |
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 C
i
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(Ag) ≤ i ≤ pos(Au) |
..120. |
AgAg. | ..120. |
AuAu. | | |
| |
| |
| |
| |
| |
| |
| |
Subtotal: 240 / 2 / 2 |
Irrep combinations (i,j) with indices: pos(Ag) ≤ i ≤ j ≤ pos(Au) |
Subtotal: 0 / 0 / 1 |
Total: 240 / 2 / 3 |
Contributions to nonvanishing cubic force field constants
Irrep combinations (i,i,i) with indices: pos(Ag) ≤ i ≤ pos(Au) |
..680. |
AgAgAg. | | |
| |
| |
| |
| |
| |
| |
| |
| |
Subtotal: 680 / 1 / 2 |
Irrep combinations (i,i,j) (i,j,j) with indices: pos(Ag) ≤ i ≤ j ≤ pos(Au) |
..1.800. |
AgAuAu. | | |
| |
| |
| |
| |
| |
| |
| |
| |
Subtotal: 1.800 / 1 / 2 |
Irrep combinations (i,j,k) with indices: pos(Ag) ≤ i ≤ j ≤ k ≤ pos(Au) |
Subtotal: 0 / 0 / 0 |
Total: 2.480 / 2 / 4 |
Contributions to nonvanishing quartic force field constants
Irrep combinations (i,i,i,i) with indices: pos(Ag) ≤ i ≤ pos(Au) |
..3.060. |
AgAgAgAg. | ..3.060. |
AuAuAuAu. | | |
| |
| |
| |
| |
| |
| |
| |
Subtotal: 6.120 / 2 / 2 |
Irrep combinations (i,i,i,j) (i,j,j,j) with indices: pos(Ag) ≤ i ≤ j ≤ pos(Au) |
Subtotal: 0 / 0 / 2 |
Irrep combinations (i,i,j,j) with indices: pos(Ag) ≤ i ≤ j ≤ pos(Au) |
..14.400. |
AgAgAuAu. | | |
| |
| |
| |
| |
| |
| |
| |
| |
Subtotal: 14.400 / 1 / 1 |
Irrep combinations (i,i,j,k) (i,j,j,k) (i,j,k,k) with indices: pos(Ag) ≤ i ≤ j ≤ k ≤ pos(Au) |
Subtotal: 0 / 0 / 0 |
Irrep combinations (i,j,k,l) with indices: pos(Ag) ≤ i ≤ j ≤ k ≤ l ≤ pos(Au) |
Subtotal: 0 / 0 / 0 |
Total: 20.520 / 3 / 5 |
Calculate contributions to
Last update November, 13th 2023 by A. Gelessus, Impressum, Datenschutzerklärung/DataPrivacyStatement