Results for Point Group D3h



Characters of representations for molecular motions
Motion E 2C3 3C'2 σh 2S3 v
Cartesian 3N 36 0 -4 12 0 4
Translation (x,y,z) 3 0 -1 1 -2 1
Rotation (Rx,Ry,Rz) 3 0 -1 -1 2 -1
Vibration 30 0 -2 12 0 4


Decomposition to irreducible representations
Motion A'1 A'2 E' A''1 A''2 E'' Total
Cartesian 3N 4 4 8 0 4 4 24
Translation (x,y,z) 0 0 1 0 1 0 2
Rotation (Rx,Ry,Rz) 0 1 0 0 0 1 2
Vibration 4 3 7 0 3 3 20



Molecular parameter
Number of Atoms (N) 12
Number of internal coordinates 30
Number of independant internal coordinates 4
Number of vibrational modes 20


Force field analysis


Allowed / forbidden vibronational transitions
Operator A'1 A'2 E' A''1 A''2 E'' Total
Linear (IR) 4 3 7 0 3 3 10 / 10
Quadratic (Raman) 4 3 7 0 3 3 14 / 6
IR + Raman - - - - 3 7 0 - - - - - - - - 7 / 3


Characters of force fields
(Symmetric powers of vibration representation)
Force field E 2C3 3C'2 σh 2S3 v
linear 30 0 -2 12 0 4
quadratic 465 0 17 87 0 23
cubic 4.960 10 -32 472 4 72
quartic 40.920 0 152 2.112 0 256
quintic 278.256 0 -272 8.184 0 680
sextic 1.623.160 55 952 28.336 13 1.904


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 3 7 0 3 3
quadratic 56 36 92 30 33 63
cubic 465 445 903 349 401 747
quartic 3.688 3.484 7.172 3.208 3.260 6.468
quintic 23.972 23.768 47.740 22.268 22.744 45.012
sextic 138.350 136.922 275.238 132.671 133.147 265.797


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...6. A'2A'2...28. E'E'...6. A''2A''2...6. E''E''.
Subtotal: 56 / 5 / 6
Irrep combinations (i,j) with indices: pos(A'1) ≤ i ≤ j ≤ pos(E'')
Subtotal: 0 / 0 / 15
Total: 56 / 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...84. E'E'E'.
Subtotal: 104 / 2 / 6
Irrep combinations (i,i,j) (i,j,j) with indices: pos(A'1) ≤ i ≤ j ≤ pos(E'')
..24. A'1A'2A'2...112. A'1E'E'...24. A'1A''2A''2...24. A'1E''E''...63. A'2E'E'...9. A'2E''E''...42. E'E''E''.
Subtotal: 298 / 7 / 30
Irrep combinations (i,j,k) with indices: pos(A'1) ≤ i ≤ j ≤ k ≤ pos(E'')
..63. E'A''2E''.
Subtotal: 63 / 1 / 20
Total: 465 / 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...15. A'2A'2A'2A'2...406. E'E'E'E'...15. A''2A''2A''2A''2...21. E''E''E''E''.
Subtotal: 492 / 5 / 6
Irrep combinations (i,i,i,j) (i,j,j,j) with indices: pos(A'1) ≤ i ≤ j ≤ pos(E'')
..336. A'1E'E'E'...252. A'2E'E'E'...30. A''2E''E''E''.
Subtotal: 618 / 3 / 30
Irrep combinations (i,i,j,j) with indices: pos(A'1) ≤ i ≤ j ≤ pos(E'')
..60. A'1A'1A'2A'2...280. A'1A'1E'E'...60. A'1A'1A''2A''2...60. A'1A'1E''E''...168. A'2A'2E'E'...36. A'2A'2A''2A''2...36. A'2A'2E''E''...168. E'E'A''2A''2...399. E'E'E''E''...36. A''2A''2E''E''.
Subtotal: 1.303 / 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''...252. A'1A'2E'E'...36. A'1A'2E''E''...168. A'1E'E''E''...126. A'2E'E''E''.
Subtotal: 834 / 5 / 60
Irrep combinations (i,j,k,l) with indices: pos(A'1) ≤ i ≤ j ≤ k ≤ l ≤ pos(E'')
..252. A'1E'A''2E''...189. A'2E'A''2E''.
Subtotal: 441 / 2 / 15
Total: 3.688 / 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