Reduction formula for point group C6v



Characters for molecular motions
Motion E 2C6 (z) 2C3 (z) C2 (z) 3v 3d
Cartesian 3N 15 10 0 -5 5 5
Translation (x,y,z) 3 2 0 -1 1 1
Rotation (Rx,Ry)* 2 1 -1 -2 0 0
Vibration 10 7 1 -2 4 4
* Linear molecule


Decomposition into Irreducible representations
Motion A1 A2 B1 B2 E1 E2 Total
Cartesian 3N 5 0 0 0 5 0 10
Translation (x,y,z) 1 0 0 0 1 0 2
Rotation (Rx,Ry)* 0 0 0 0 1 0 1
Vibration 4 0 0 0 3 0 7
* Linear molecule


Molecule Parameter
Number of Atoms (N) 5
Number of internal coordinates 10
Number of independant internal coordinates 4
Number of vibrational modes 7





Force field analysis


Allowed / forbidden vibronational transitions
Operator A1 A2 B1 B2 E1 E2 Total
Linear (IR) 4 0 0 0 3 0 7 / 0
Quadratic (Raman) 4 0 0 0 3 0 7 / 0
IR + Raman 4 0 0 0 3 - 7 / 0



Characters of symmetric powers for vibration representation
Force field Tensor
Order
E 2C6 (z) 2C3 (z) C2 (z) 3v 3d
linear 1 10 7 1 -2 4 4
quadratic 2 55 25 1 7 13 13
cubic 3 220 60 4 -12 32 32
quartic 4 715 108 4 27 71 71
quintic 5 2.002 156 4 -42 140 140
sextic 6 5.005 194 10 77 259 259


Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field Tensor
Order
A1 A2 B1 B2 E1 E2
linear 1 4 0 0 0 3 0
quadratic 2 16 3 0 0 12 6
cubic 3 44 12 10 10 48 24
quartic 4 116 45 40 40 132 105
quintic 5 260 120 145 145 366 300
sextic 6 587 328 380 380 852 813


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