Reduction formula for point group D2d



Characters for molecular motions
Motion E 2S4 C2 (z) 2C'2 2d
Cartesian 3N 48 0 0 0 8
Translation (x,y,z) 3 -1 -1 -1 1
Rotation (Rx,Ry,Rz) 3 1 -1 -1 -1
Vibration 42 0 2 2 8



Decomposition into Irreducible representations
Motion A1 A2 B1 B2 E Total
Cartesian 3N 8 4 4 8 12 36
Translation (x,y,z) 0 0 0 1 1 2
Rotation (Rx,Ry,Rz) 0 1 0 0 1 2
Vibration 8 3 4 7 10 32



Molecule Parameter
Number of Atoms (N) 16
Number of internal coordinates 42
Number of independant internal coordinates 8
Number of vibrational modes 32





Force field analysis


Allowed / forbidden vibronational transitions
Operator A1 A2 B1 B2 E Total
Linear (IR) 8 3 4 7 10 17 / 15
Quadratic (Raman) 8 3 4 7 10 29 / 3
IR + Raman - 3 - 7 10 17 / 3



Characters of symmetric powers for vibration representation
Force field Tensor
Order
E 2S4 C2 (z) 2C'2 2d
linear 1 42 0 2 2 8
quadratic 2 903 1 23 23 53
cubic 3 13.244 0 44 44 256
quartic 4 148.995 11 275 275 1.095
quintic 5 1.370.754 0 506 506 4.056
sextic 6 10.737.573 11 2.277 2.277 13.803


Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field Tensor
Order
A1 A2 B1 B2 E
linear 1 8 3 4 7 10
quadratic 2 135 97 108 123 220
cubic 3 1.736 1.586 1.608 1.714 3.300
quartic 4 19.004 18.319 18.451 18.861 37.180
quintic 5 172.548 170.267 170.520 172.295 342.562
sextic 6 1.346.504 1.338.464 1.339.597 1.345.360 2.683.824


Literature




Character tables for chemically important point groups Character table for point group D2d Constructor University Bremen

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