Reduction formula for point group C6v



Characters for molecular motions
Motion E 2C6 (z) 2C3 (z) C2 (z) 3v 3d
Cartesian 3N 18 12 0 -6 6 6
Translation (x,y,z) 3 2 0 -1 1 1
Rotation (Rx,Ry)* 2 1 -1 -2 0 0
Vibration 13 9 1 -3 5 5
* Linear molecule


Decomposition into Irreducible representations
Motion A1 A2 B1 B2 E1 E2 Total
Cartesian 3N 6 0 0 0 6 0 12
Translation (x,y,z) 1 0 0 0 1 0 2
Rotation (Rx,Ry)* 0 0 0 0 1 0 1
Vibration 5 0 0 0 4 0 9
* Linear molecule


Molecule Parameter
Number of Atoms (N) 6
Number of internal coordinates 13
Number of independant internal coordinates 5
Number of vibrational modes 9





Force field analysis


Allowed / forbidden vibronational transitions
Operator A1 A2 B1 B2 E1 E2 Total
Linear (IR) 5 0 0 0 4 0 9 / 0
Quadratic (Raman) 5 0 0 0 4 0 9 / 0
IR + Raman 5 0 0 0 4 - 9 / 0



Characters of symmetric powers for vibration representation
Force field Tensor
Order
E 2C6 (z) 2C3 (z) C2 (z) 3v 3d
linear 1 13 9 1 -3 5 5
quadratic 2 91 41 1 11 19 19
cubic 3 455 125 5 -25 55 55
quartic 4 1.820 285 5 60 140 140
quintic 5 6.188 517 5 -116 316 316
sextic 6 18.564 783 15 228 660 660


Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field Tensor
Order
A1 A2 B1 B2 E1 E2
linear 1 5 0 0 0 4 0
quadratic 2 25 6 0 0 20 10
cubic 3 85 30 20 20 100 50
quartic 4 275 135 100 100 340 265
quintic 5 751 435 440 440 1.136 925
sextic 6 2.029 1.369 1.400 1.400 3.184 2.999


Literature




Character tables for chemically important point groups Character table for point group C6v Constructor University Bremen

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