Reduction formula for point group C4v



Characters for molecular motions
Motion E 2C4 (z) C2 2v 2d
Cartesian 3N 99 1 -1 5 5
Translation (x,y,z) 3 1 -1 1 1
Rotation (Rx,Ry,Rz) 3 1 -1 -1 -1
Vibration 93 -1 1 5 5



Decomposition into Irreducible representations
Motion A1 A2 B1 B2 E Total
Cartesian 3N 15 10 12 12 25 74
Translation (x,y,z) 1 0 0 0 1 2
Rotation (Rx,Ry,Rz) 0 1 0 0 1 2
Vibration 14 9 12 12 23 70



Molecule Parameter
Number of Atoms (N) 33
Number of internal coordinates 93
Number of independant internal coordinates 14
Number of vibrational modes 70





Force field analysis


Allowed / forbidden vibronational transitions
Operator A1 A2 B1 B2 E Total
Linear (IR) 14 9 12 12 23 37 / 33
Quadratic (Raman) 14 9 12 12 23 61 / 9
IR + Raman 14 9 - - 23 37 / 9



Characters of symmetric powers for vibration representation
Force field Tensor
Order
E 2C4 (z) C2 2v 2d
linear 1 93 -1 1 5 5
quadratic 2 4.371 1 47 59 59
cubic 3 138.415 -1 47 255 255
quartic 4 3.321.960 24 1.128 1.720 1.720
quintic 5 64.446.024 -24 1.128 6.616 6.616
sextic 6 1.052.618.392 24 18.424 33.320 33.320


Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field Tensor
Order
A1 A2 B1 B2 E
linear 1 14 9 12 12 23
quadratic 2 582 523 552 552 1.081
cubic 3 17.435 17.180 17.308 17.308 34.592
quartic 4 416.252 414.532 415.380 415.380 830.208
quintic 5 8.059.196 8.052.580 8.055.900 8.055.900 16.111.224
sextic 6 131.596.268 131.562.948 131.579.596 131.579.596 263.149.992


Literature




Character tables for chemically important point groups Character table for point group C4v Constructor University Bremen

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