Reduction formula for point group D3d



Characters for molecular motions
Motion E 2C3 3C'2 i 2S6 3d
Cartesian 3N 21 0 -1 -3 0 3
Translation (x,y,z) 3 0 -1 -3 0 1
Rotation (Rx,Ry,Rz) 3 0 -1 3 0 -1
Vibration 15 0 1 -3 0 3



Decomposition into Irreducible representations
Motion A1g A2g Eg A1u A2u Eu Total
Cartesian 3N 2 1 3 1 3 4 14
Translation (x,y,z) 0 0 0 0 1 1 2
Rotation (Rx,Ry,Rz) 0 1 1 0 0 0 2
Vibration 2 0 2 1 2 3 10



Molecule Parameter
Number of Atoms (N) 7
Number of internal coordinates 15
Number of independant internal coordinates 2
Number of vibrational modes 10





Force field analysis


Allowed / forbidden vibronational transitions
Operator A1g A2g Eg A1u A2u Eu Total
Linear (IR) 2 0 2 1 2 3 5 / 5
Quadratic (Raman) 2 0 2 1 2 3 4 / 6
IR + Raman - 0 - 1 - - 0* / 1
* Center of inversion: Mutual Exclusion Principle



Characters of symmetric powers for vibration representation
Force field Tensor
Order
E 2C3 3C'2 i 2S6 3d
linear 1 15 0 1 -3 0 3
quadratic 2 120 0 8 12 0 12
cubic 3 680 5 8 -28 -1 28
quartic 4 3.060 0 36 72 0 72
quintic 5 11.628 0 36 -144 0 144
sextic 6 38.760 15 120 300 3 300


Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field Tensor
Order
A1g A2g Eg A1u A2u Eu
linear 1 2 0 2 1 2 3
quadratic 2 16 6 22 8 10 18
cubic 3 64 46 108 55 65 117
quartic 4 288 234 522 240 258 498
quintic 5 1.002 912 1.914 954 1.008 1.962
sextic 6 3.363 3.153 6.507 3.162 3.252 6.408


Literature




Character tables for chemically important point groups Character table for point group D3d Constructor University Bremen

Last update November, 13th 2023 by A. Gelessus, Impressum, Datenschutzerklärung/DataPrivacyStatement