Reduction formula for point group C2v



Characters for molecular motions
Motion E C2 (z) v(xz) v(yz)
Cartesian 3N 60 0 4 4
Translation (x,y,z) 3 -1 1 1
Rotation (Rx,Ry,Rz) 3 -1 -1 -1
Vibration 54 2 4 4



Decomposition into Irreducible representations
Motion A1 A2 B1 B2 Total
Cartesian 3N 17 13 15 15 60
Translation (x,y,z) 1 0 1 1 3
Rotation (Rx,Ry,Rz) 0 1 1 1 3
Vibration 16 12 13 13 54



Molecule Parameter
Number of Atoms (N) 20
Number of internal coordinates 54
Number of independant internal coordinates 16
Number of vibrational modes 54





Force field analysis


Allowed / forbidden vibronational transitions
Operator A1 A2 B1 B2 Total
Linear (IR) 16 12 13 13 42 / 12
Quadratic (Raman) 16 12 13 13 54 / 0
IR + Raman 16 - 13 13 42 / 0



Characters of symmetric powers for vibration representation
Force field Tensor
Order
E C2 (z) v(xz) v(yz)
linear 1 54 2 4 4
quadratic 2 1.485 29 35 35
cubic 3 27.720 56 120 120
quartic 4 395.010 434 610 610
quintic 5 4.582.116 812 1.856 1.856
sextic 6 45.057.474 4.466 7.134 7.134


Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field Tensor
Order
A1 A2 B1 B2
linear 1 16 12 13 13
quadratic 2 396 361 364 364
cubic 3 7.004 6.884 6.916 6.916
quartic 4 99.166 98.556 98.644 98.644
quintic 5 1.146.660 1.144.804 1.145.326 1.145.326
sextic 6 11.269.052 11.261.918 11.263.252 11.263.252


Literature




Character tables for chemically important point groups Character table for point group C2v Constructor University Bremen

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