Reduction formula for point group C4v



Characters for molecular motions
Motion E 2C4 (z) C2 2v 2d
Cartesian 3N 99 1 -1 9 9
Translation (x,y,z) 3 1 -1 1 1
Rotation (Rx,Ry,Rz) 3 1 -1 -1 -1
Vibration 93 -1 1 9 9



Decomposition into Irreducible representations
Motion A1 A2 B1 B2 E Total
Cartesian 3N 17 8 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 16 7 12 12 23 70



Molecule Parameter
Number of Atoms (N) 33
Number of internal coordinates 93
Number of independant internal coordinates 16
Number of vibrational modes 70





Force field analysis


Allowed / forbidden vibronational transitions
Operator A1 A2 B1 B2 E Total
Linear (IR) 16 7 12 12 23 39 / 31
Quadratic (Raman) 16 7 12 12 23 63 / 7
IR + Raman 16 7 - - 23 39 / 7



Characters of symmetric powers for vibration representation
Force field Tensor
Order
E 2C4 (z) C2 2v 2d
linear 1 93 -1 1 9 9
quadratic 2 4.371 1 47 87 87
cubic 3 138.415 -1 47 543 543
quartic 4 3.321.960 24 1.128 3.288 3.288
quintic 5 64.446.024 -24 1.128 16.344 16.344
sextic 6 1.052.618.392 24 18.424 77.672 77.672


Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field Tensor
Order
A1 A2 B1 B2 E
linear 1 16 7 12 12 23
quadratic 2 596 509 552 552 1.081
cubic 3 17.579 17.036 17.308 17.308 34.592
quartic 4 417.036 413.748 415.380 415.380 830.208
quintic 5 8.064.060 8.047.716 8.055.900 8.055.900 16.111.224
sextic 6 131.618.444 131.540.772 131.579.596 131.579.596 263.149.992


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