Reduction formula for point group D2d



Characters for molecular motions
Motion E 2S4 C2 (z) 2C'2 2d
Cartesian 3N 84 0 0 0 6
Translation (x,y,z) 3 -1 -1 -1 1
Rotation (Rx,Ry,Rz) 3 1 -1 -1 -1
Vibration 78 0 2 2 6



Decomposition into Irreducible representations
Motion A1 A2 B1 B2 E Total
Cartesian 3N 12 9 9 12 21 63
Translation (x,y,z) 0 0 0 1 1 2
Rotation (Rx,Ry,Rz) 0 1 0 0 1 2
Vibration 12 8 9 11 19 59



Molecule Parameter
Number of Atoms (N) 28
Number of internal coordinates 78
Number of independant internal coordinates 12
Number of vibrational modes 59





Force field analysis


Allowed / forbidden vibronational transitions
Operator A1 A2 B1 B2 E Total
Linear (IR) 12 8 9 11 19 30 / 29
Quadratic (Raman) 12 8 9 11 19 51 / 8
IR + Raman - 8 - 11 19 30 / 8



Characters of symmetric powers for vibration representation
Force field Tensor
Order
E 2S4 C2 (z) 2C'2 2d
linear 1 78 0 2 2 6
quadratic 2 3.081 1 41 41 57
cubic 3 82.160 0 80 80 272
quartic 4 1.663.740 20 860 860 1.548
quintic 5 27.285.336 0 1.640 1.640 6.264
sextic 6 377.447.148 20 12.300 12.300 27.420


Decomposition into Irreducible representations
Number of nonvanshing force constants
Force field Tensor
Order
A1 A2 B1 B2 E
linear 1 12 8 9 11 19
quadratic 2 415 366 386 394 760
cubic 3 10.368 10.192 10.232 10.328 20.520
quartic 4 208.682 207.478 207.898 208.242 415.720
quintic 5 3.412.848 3.408.896 3.409.716 3.412.028 6.820.924
sextic 6 47.192.366 47.172.506 47.178.646 47.186.206 94.358.712


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