Reduction formula for point group O



Characters for molecular motions
Motion E 8C3 6C'2 6C4 3C2 =(C4)2
Cartesian 3N 36 0 0 4 -4
Translation (x,y,z) 3 0 -1 1 -1
Rotation (Rx,Ry,Rz) 3 0 -1 1 -1
Vibration 30 0 2 2 -2



Decomposition into Irreducible representations
Motion A1 A2 E T1 T2 Total
Cartesian 3N 2 0 2 6 4 14
Translation (x,y,z) 0 0 0 1 0 1
Rotation (Rx,Ry,Rz) 0 0 0 1 0 1
Vibration 2 0 2 4 4 12



Molecule Parameter
Number of Atoms (N) 12
Number of internal coordinates 30
Number of independant internal coordinates 2
Number of vibrational modes 12





Force field analysis


Allowed / forbidden vibronational transitions
Operator A1 A2 E T1 T2 Total
Linear (IR) 2 0 2 4 4 4 / 8
Quadratic (Raman) 2 0 2 4 4 8 / 4
IR + Raman - 0 - - - 0 / 0



Characters of symmetric powers for vibration representation
Force field Tensor
Order
E 8C3 6C'2 6C4 3C2 =(C4)2
linear 1 30 0 2 2 -2
quadratic 2 465 0 17 1 17
cubic 3 4.960 10 32 0 -32
quartic 4 40.920 0 152 8 152
quintic 5 278.256 0 272 16 -272
sextic 6 1.623.160 55 952 8 952


Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field Tensor
Order
A1 A2 E T1 T2
linear 1 2 0 2 4 4
quadratic 2 26 17 43 52 60
cubic 3 214 198 402 616 632
quartic 4 1.764 1.684 3.448 5.060 5.132
quintic 5 11.632 11.488 23.120 34.752 34.880
sextic 6 68.009 67.529 135.483 202.540 203.012


Literature




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

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