Results for Point Group D4d



Characters of representations for molecular motions
Motion E 2S8 2C4 2(S8)3 C2 4C'2 d
Cartesian 3N 24 0.000 0 -0.000 0 0 2
Translation (x,y,z) 3 0.414 1 -2.414 -1 -1 1
Rotation (Rx,Ry,Rz) 3 -0.414 1 2.414 -1 -1 -1
Vibration 18 0.000 -2 0.000 2 2 2


Decomposition to irreducible representations
Motion A1 A2 B1 B2 E1 E2 E3 Total
Cartesian 3N 2 1 1 2 3 3 3 15
Translation (x,y,z) 0 0 0 1 1 0 0 2
Rotation (Rx,Ry,Rz) 0 1 0 0 0 0 1 2
Vibration 2 0 1 1 2 3 2 11



Molecular parameter
Number of Atoms (N) 8
Number of internal coordinates 18
Number of independant internal coordinates 2
Number of vibrational modes 11


Force field analysis


Allowed / forbidden vibronational transitions
Operator A1 A2 B1 B2 E1 E2 E3 Total
Linear (IR) 2 0 1 1 2 3 2 3 / 8
Quadratic (Raman) 2 0 1 1 2 3 2 7 / 4
IR + Raman - - - - 0 1 - - - - - - - - - - - - - - - - 0 / 1


Characters of force fields
(Symmetric powers of vibration representation)
Force field E 2S8 2C4 2(S8)3 C2 4C'2 d
linear 18 0.000 -2 0.000 2 2 2
quadratic 171 -1.000 3 -1.000 11 11 11
cubic 1.140 -0.000 -4 -0.000 20 20 20
quartic 5.985 1.000 9 1.000 65 65 65
quintic 26.334 0.000 -14 0.000 110 110 110
sextic 100.947 -1.000 19 -1.000 275 275 275


Decomposition to irreducible representations
Column with number of nonvanshing force constants highlighted
Force field A1 A2 B1 B2 E1 E2 E3
linear 2 0 1 1 2 3 2
quadratic 17 6 12 12 20 22 20
cubic 82 62 72 72 140 146 140
quartic 412 347 379 379 740 754 740
quintic 1.706 1.596 1.651 1.651 3.278 3.309 3.278
sextic 6.466 6.191 6.329 6.329 12.584 12.648 12.584


Further Reading



Contributions to nonvanishing force field constants


pos(X) : Position of irreducible representation (irrep) X in character table of D4d

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(E3)
..3. A1A1...1. B1B1...1. B2B2...3. E1E1...6. E2E2...3. E3E3.
Subtotal: 17 / 6 / 7
Irrep combinations (i,j) with indices: pos(A1) ≤ i ≤ j ≤ pos(E3)
Subtotal: 0 / 0 / 21
Total: 17 / 6 / 28


Contributions to nonvanishing cubic force field constants
Irrep combinations (i,i,i) with indices: pos(A1) ≤ i ≤ pos(E3)
..4. A1A1A1.
Subtotal: 4 / 1 / 7
Irrep combinations (i,i,j) (i,j,j) with indices: pos(A1) ≤ i ≤ j ≤ pos(E3)
..9. E1E1E2...2. A1B1B1...2. A1B2B2...6. A1E1E1...12. A1E2E2...6. A1E3E3...6. B1E2E2...6. B2E2E2...9. E2E3E3.
Subtotal: 58 / 9 / 42
Irrep combinations (i,j,k) with indices: pos(A1) ≤ i ≤ j ≤ k ≤ pos(E3)
..4. B1E1E3...4. B2E1E3...12. E1E2E3.
Subtotal: 20 / 3 / 35
Total: 82 / 13 / 84


Contributions to nonvanishing quartic force field constants
Irrep combinations (i,i,i,i) with indices: pos(A1) ≤ i ≤ pos(E3)
..5. A1A1A1A1...1. B1B1B1B1...1. B2B2B2B2...6. E1E1E1E1...36. E2E2E2E2...6. E3E3E3E3.
Subtotal: 55 / 6 / 7
Irrep combinations (i,i,i,j) (i,j,j,j) with indices: pos(A1) ≤ i ≤ j ≤ pos(E3)
..8. E1E1E1E3...8. E1E3E3E3.
Subtotal: 16 / 2 / 42
Irrep combinations (i,i,j,j) with indices: pos(A1) ≤ i ≤ j ≤ pos(E3)
..3. A1A1B1B1...3. A1A1B2B2...9. A1A1E1E1...18. A1A1E2E2...9. A1A1E3E3...1. B1B1B2B2...3. B1B1E1E1...6. B1B1E2E2...3. B1B1E3E3...3. B2B2E1E1.
..6. B2B2E2E2...3. B2B2E3E3...21. E1E1E2E2...19. E1E1E3E3...21. E2E2E3E3.
Subtotal: 128 / 15 / 21
Irrep combinations (i,i,j,k) (i,j,j,k) (i,j,k,k) with indices: pos(A1) ≤ i ≤ j ≤ k ≤ pos(E3)
..18. A1E1E1E2...9. B1E1E1E2...9. B2E1E1E2...48. E1E2E2E3...12. A1B1E2E2...12. A1B2E2E2...18. A1E2E3E3...1. B1B2E1E1...3. B1B2E2E2...1. B1B2E3E3.
..9. B1E2E3E3...9. B2E2E3E3.
Subtotal: 149 / 12 / 105
Irrep combinations (i,j,k,l) with indices: pos(A1) ≤ i ≤ j ≤ k ≤ l ≤ pos(E3)
..8. A1B1E1E3...8. A1B2E1E3...24. A1E1E2E3...12. B1E1E2E3...12. B2E1E2E3.
Subtotal: 64 / 5 / 35
Total: 412 / 40 / 210


Calculate contributions to

A1 A2 B1 B2 E1 E2 E3
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Last update November, 13th 2023 by A. Gelessus, Impressum, Datenschutzerklärung/DataPrivacyStatement