Reduction formula for point group C6v



Characters for molecular motions
Motion E 2C6 (z) 2C3 (z) C2 (z) 3v 3d
Cartesian 3N 36 0 0 0 0 4
Translation (x,y,z) 3 2 0 -1 1 1
Rotation (Rx,Ry,Rz) 3 2 0 -1 -1 -1
Vibration 30 -4 0 2 0 4



Decomposition into Irreducible representations
Motion A1 A2 B1 B2 E1 E2 Total
Cartesian 3N 4 2 2 4 6 6 24
Translation (x,y,z) 1 0 0 0 1 0 2
Rotation (Rx,Ry,Rz) 0 1 0 0 1 0 2
Vibration 3 1 2 4 4 6 20



Molecule Parameter
Number of Atoms (N) 12
Number of internal coordinates 30
Number of independant internal coordinates 3
Number of vibrational modes 20





Force field analysis


Allowed / forbidden vibronational transitions
Operator A1 A2 B1 B2 E1 E2 Total
Linear (IR) 3 1 2 4 4 6 7 / 13
Quadratic (Raman) 3 1 2 4 4 6 13 / 7
IR + Raman 3 1 2 4 4 - 7 / 7



Characters of symmetric powers for vibration representation
Force field Tensor
Order
E 2C6 (z) 2C3 (z) C2 (z) 3v 3d
linear 1 30 -4 0 2 0 4
quadratic 2 465 8 0 17 15 23
cubic 3 4.960 -10 10 32 0 72
quartic 4 40.920 8 0 152 120 256
quintic 5 278.256 -4 0 272 0 680
sextic 6 1.623.160 7 55 952 680 1.904


Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field Tensor
Order
A1 A2 B1 B2 E1 E2
linear 1 3 1 2 4 4 6
quadratic 2 51 32 34 38 76 79
cubic 3 434 398 396 432 818 832
quartic 4 3.518 3.330 3.362 3.430 6.796 6.844
quintic 5 23.380 23.040 22.996 23.336 46.330 46.422
sextic 6 135.999 134.707 134.886 135.498 270.360 270.675


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