Reduction formula for point group D2d



Characters for molecular motions
Motion E 2S4 C2 (z) 2C'2 2d
Cartesian 3N 12 0 0 -2 0
Translation (x,y,z) 3 -1 -1 -1 1
Rotation (Rx,Ry,Rz) 3 1 -1 -1 -1
Vibration 6 0 2 0 0



Decomposition into Irreducible representations
Motion A1 A2 B1 B2 E Total
Cartesian 3N 1 2 1 2 3 9
Translation (x,y,z) 0 0 0 1 1 2
Rotation (Rx,Ry,Rz) 0 1 0 0 1 2
Vibration 1 1 1 1 1 5



Molecule Parameter
Number of Atoms (N) 4
Number of internal coordinates 6
Number of independant internal coordinates 1
Number of vibrational modes 5





Force field analysis


Allowed / forbidden vibronational transitions
Operator A1 A2 B1 B2 E Total
Linear (IR) 1 1 1 1 1 2 / 3
Quadratic (Raman) 1 1 1 1 1 4 / 1
IR + Raman - 1 - 1 1 2 / 1



Characters of symmetric powers for vibration representation
Force field Tensor
Order
E 2S4 C2 (z) 2C'2 2d
linear 1 6 0 2 0 0
quadratic 2 21 1 5 3 3
cubic 3 56 0 8 0 0
quartic 4 126 2 14 6 6
quintic 5 252 0 20 0 0
sextic 6 462 2 30 10 10


Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field Tensor
Order
A1 A2 B1 B2 E
linear 1 1 1 1 1 1
quadratic 2 5 2 3 3 4
cubic 3 8 8 8 8 12
quartic 4 21 15 17 17 28
quintic 5 34 34 34 34 58
sextic 6 67 57 61 61 108


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