Reduction formula for point group D2d



Characters for molecular motions
Motion E 2S4 C2 (z) 2C'2 2d
Cartesian 3N 75 -1 -1 -1 5
Translation (x,y,z) 3 -1 -1 -1 1
Rotation (Rx,Ry,Rz) 3 1 -1 -1 -1
Vibration 69 -1 1 1 5



Decomposition into Irreducible representations
Motion A1 A2 B1 B2 E Total
Cartesian 3N 10 8 8 11 19 56
Translation (x,y,z) 0 0 0 1 1 2
Rotation (Rx,Ry,Rz) 0 1 0 0 1 2
Vibration 10 7 8 10 17 52



Molecule Parameter
Number of Atoms (N) 25
Number of internal coordinates 69
Number of independant internal coordinates 10
Number of vibrational modes 52





Force field analysis


Allowed / forbidden vibronational transitions
Operator A1 A2 B1 B2 E Total
Linear (IR) 10 7 8 10 17 27 / 25
Quadratic (Raman) 10 7 8 10 17 45 / 7
IR + Raman - 7 - 10 17 27 / 7



Characters of symmetric powers for vibration representation
Force field Tensor
Order
E 2S4 C2 (z) 2C'2 2d
linear 1 69 -1 1 1 5
quadratic 2 2.415 1 35 35 47
cubic 3 57.155 -1 35 35 195
quartic 4 1.028.790 18 630 630 1.078
quintic 5 15.020.334 -18 630 630 3.886
sextic 6 185.250.786 18 7.770 7.770 16.354


Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field Tensor
Order
A1 A2 B1 B2 E
linear 1 10 7 8 10 17
quadratic 2 327 286 303 309 595
cubic 3 7.206 7.091 7.109 7.189 14.280
quartic 4 129.109 128.255 128.561 128.785 257.040
quintic 5 1.878.745 1.876.487 1.876.811 1.878.439 3.754.926
sextic 6 23.163.355 23.151.293 23.155.169 23.159.461 46.310.754


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