Reduction formula for point group O



Characters for molecular motions
Motion E 8C3 6C'2 6C4 3C2 =(C4)2
Cartesian 3N 39 0 -1 5 -5
Translation (x,y,z) 3 0 -1 1 -1
Rotation (Rx,Ry,Rz) 3 0 -1 1 -1
Vibration 33 0 1 3 -3



Decomposition into Irreducible representations
Motion A1 A2 E T1 T2 Total
Cartesian 3N 2 0 2 7 4 15
Translation (x,y,z) 0 0 0 1 0 1
Rotation (Rx,Ry,Rz) 0 0 0 1 0 1
Vibration 2 0 2 5 4 13



Molecule Parameter
Number of Atoms (N) 13
Number of internal coordinates 33
Number of independant internal coordinates 2
Number of vibrational modes 13





Force field analysis


Allowed / forbidden vibronational transitions
Operator A1 A2 E T1 T2 Total
Linear (IR) 2 0 2 5 4 5 / 8
Quadratic (Raman) 2 0 2 5 4 8 / 5
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 33 0 1 3 -3
quadratic 2 561 0 17 3 21
cubic 3 6.545 11 17 1 -55
quartic 4 58.905 0 153 9 225
quintic 5 435.897 0 153 27 -531
sextic 6 2.760.681 66 969 27 1.653


Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field Tensor
Order
A1 A2 E T1 T2
linear 1 2 0 2 5 4
quadratic 2 31 21 52 64 71
cubic 3 274 265 528 821 829
quartic 4 2.523 2.442 4.965 7.299 7.371
quintic 5 18.141 18.051 36.192 54.522 54.585
sextic 6 115.506 115.008 230.448 344.643 345.114


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