Results for Point Group D3h



Characters of representations for molecular motions
Motion E 2C3 3C'2 σh 2S3 v
Cartesian 3N 33 0 -3 7 -2 7
Translation (x,y,z) 3 0 -1 1 -2 1
Rotation (Rx,Ry,Rz) 3 0 -1 -1 2 -1
Vibration 27 0 -1 7 -2 7


Decomposition to irreducible representations
Motion A'1 A'2 E' A''1 A''2 E'' Total
Cartesian 3N 4 2 7 0 5 4 22
Translation (x,y,z) 0 0 1 0 1 0 2
Rotation (Rx,Ry,Rz) 0 1 0 0 0 1 2
Vibration 4 1 6 0 4 3 18



Molecular parameter
Number of Atoms (N) 11
Number of internal coordinates 27
Number of independant internal coordinates 4
Number of vibrational modes 18


Force field analysis


Allowed / forbidden vibronational transitions
Operator A'1 A'2 E' A''1 A''2 E'' Total
Linear (IR) 4 1 6 0 4 3 10 / 8
Quadratic (Raman) 4 1 6 0 4 3 13 / 5
IR + Raman - - - - 1 6 0 - - - - - - - - 6 / 1


Characters of force fields
(Symmetric powers of vibration representation)
Force field E 2C3 3C'2 σh 2S3 v
linear 27 0 -1 7 -2 7
quadratic 378 0 14 38 2 38
cubic 3.654 9 -14 154 1 154
quartic 27.405 0 105 545 -4 545
quintic 169.911 0 -105 1.687 4 1.687
sextic 906.192 45 560 4.784 5 4.784


Decomposition to irreducible representations
Column with number of nonvanshing force constants highlighted
Force field A'1 A'2 E' A''1 A''2 E''
linear 4 1 6 0 4 3
quadratic 48 22 69 22 34 57
cubic 354 284 633 251 335 582
quartic 2.491 2.166 4.659 2.129 2.349 4.476
quintic 14.696 13.905 28.599 13.570 14.466 28.038
sextic 77.259 74.587 151.821 74.068 76.180 150.228


Further Reading



Contributions to nonvanishing force field constants


pos(X) : Position of irreducible representation (irrep) X in character table of D3h

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(A'1) ≤ i ≤ pos(E'')
..10. A'1A'1...1. A'2A'2...21. E'E'...10. A''2A''2...6. E''E''.
Subtotal: 48 / 5 / 6
Irrep combinations (i,j) with indices: pos(A'1) ≤ i ≤ j ≤ pos(E'')
Subtotal: 0 / 0 / 15
Total: 48 / 5 / 21


Contributions to nonvanishing cubic force field constants
Irrep combinations (i,i,i) with indices: pos(A'1) ≤ i ≤ pos(E'')
..20. A'1A'1A'1...56. E'E'E'.
Subtotal: 76 / 2 / 6
Irrep combinations (i,i,j) (i,j,j) with indices: pos(A'1) ≤ i ≤ j ≤ pos(E'')
..4. A'1A'2A'2...84. A'1E'E'...40. A'1A''2A''2...24. A'1E''E''...15. A'2E'E'...3. A'2E''E''...36. E'E''E''.
Subtotal: 206 / 7 / 30
Irrep combinations (i,j,k) with indices: pos(A'1) ≤ i ≤ j ≤ k ≤ pos(E'')
..72. E'A''2E''.
Subtotal: 72 / 1 / 20
Total: 354 / 10 / 56


Contributions to nonvanishing quartic force field constants
Irrep combinations (i,i,i,i) with indices: pos(A'1) ≤ i ≤ pos(E'')
..35. A'1A'1A'1A'1...1. A'2A'2A'2A'2...231. E'E'E'E'...35. A''2A''2A''2A''2...21. E''E''E''E''.
Subtotal: 323 / 5 / 6
Irrep combinations (i,i,i,j) (i,j,j,j) with indices: pos(A'1) ≤ i ≤ j ≤ pos(E'')
..224. A'1E'E'E'...56. A'2E'E'E'...40. A''2E''E''E''.
Subtotal: 320 / 3 / 30
Irrep combinations (i,i,j,j) with indices: pos(A'1) ≤ i ≤ j ≤ pos(E'')
..10. A'1A'1A'2A'2...210. A'1A'1E'E'...100. A'1A'1A''2A''2...60. A'1A'1E''E''...21. A'2A'2E'E'...10. A'2A'2A''2A''2...6. A'2A'2E''E''...210. E'E'A''2A''2...297. E'E'E''E''...60. A''2A''2E''E''.
Subtotal: 984 / 10 / 15
Irrep combinations (i,i,j,k) (i,j,j,k) (i,j,k,k) with indices: pos(A'1) ≤ i ≤ j ≤ k ≤ pos(E'')
..252. E'E'A''2E''...60. A'1A'2E'E'...12. A'1A'2E''E''...144. A'1E'E''E''...36. A'2E'E''E''.
Subtotal: 504 / 5 / 60
Irrep combinations (i,j,k,l) with indices: pos(A'1) ≤ i ≤ j ≤ k ≤ l ≤ pos(E'')
..288. A'1E'A''2E''...72. A'2E'A''2E''.
Subtotal: 360 / 2 / 15
Total: 2.491 / 25 / 126


Calculate contributions to

A'1 A'2 E' A''1 A''2 E''
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Last update November, 13th 2023 by A. Gelessus, Impressum, Datenschutzerklärung/DataPrivacyStatement