Results for Point Group D5d



Characters of representations for molecular motions
Motion E 2C5 2(C5)2 5C'2 i 2(S10)3 2S10 d
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 d
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



Contributions to nonvanishing force field constants


pos(X) : Position of irreducible representation (irrep) X in character table of D5d

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


Calculate contributions to

A1g A2g E1g E2g A1u A2u E1u E2u
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Last update November, 13th 2023 by A. Gelessus, Impressum, Datenschutzerklärung/DataPrivacyStatement