Results for Point Group Cs



Characters of representations for molecular motions
Motion E σh
Cartesian 3N 48 8
Translation (x,y,z) 3 1
Rotation (Rx,Ry,Rz) 3 -1
Vibration 42 8


Decomposition to irreducible representations
Motion A' A'' Total
Cartesian 3N 28 20 48
Translation (x,y,z) 2 1 3
Rotation (Rx,Ry,Rz) 1 2 3
Vibration 25 17 42



Molecular parameter
Number of Atoms (N) 16
Number of internal coordinates 42
Number of independant internal coordinates 25
Number of vibrational modes 42


Force field analysis


Allowed / forbidden vibronational transitions
Operator A' A'' Total
Linear (IR) 25 17 42 / 0
Quadratic (Raman) 25 17 42 / 0
IR + Raman 25 17 42 / 0


Characters of force fields
(Symmetric powers of vibration representation)
Force field E σh
linear 42 8
quadratic 903 53
cubic 13.244 256
quartic 148.995 1.095
quintic 1.370.754 4.056
sextic 10.737.573 13.803


Decomposition to irreducible representations
Column with number of nonvanshing force constants highlighted
Force field A' A''
linear 25 17
quadratic 478 425
cubic 6.750 6.494
quartic 75.045 73.950
quintic 687.405 683.349
sextic 5.375.688 5.361.885


Further Reading



Contributions to nonvanishing force field constants


pos(X) : Position of irreducible representation (irrep) X in character table of Cs

Subtotal: <Number of nonvanishing force constants in subsection> / <number of nonzero irrep combinations in subsection> / <number of irrep combinations in subsection>
Total: <Number of nonvanishing force constants in force field> / <number of nonzero irrep combinations in force field> / <number of irrep combinations in force field>


Contributions to nonvanishing quadratic force field constants
Irrep combinations (i,i) with indices: pos(A') ≤ i ≤ pos(A'')
..325. A'A'...153. A''A''.
Subtotal: 478 / 2 / 2
Irrep combinations (i,j) with indices: pos(A') ≤ i ≤ j ≤ pos(A'')
Subtotal: 0 / 0 / 1
Total: 478 / 2 / 3


Contributions to nonvanishing cubic force field constants
Irrep combinations (i,i,i) with indices: pos(A') ≤ i ≤ pos(A'')
..2.925. A'A'A'.
Subtotal: 2.925 / 1 / 2
Irrep combinations (i,i,j) (i,j,j) with indices: pos(A') ≤ i ≤ j ≤ pos(A'')
..3.825. A'A''A''.
Subtotal: 3.825 / 1 / 2
Irrep combinations (i,j,k) with indices: pos(A') ≤ i ≤ j ≤ k ≤ pos(A'')
Subtotal: 0 / 0 / 0
Total: 6.750 / 2 / 4


Contributions to nonvanishing quartic force field constants
Irrep combinations (i,i,i,i) with indices: pos(A') ≤ i ≤ pos(A'')
..20.475. A'A'A'A'...4.845. A''A''A''A''.
Subtotal: 25.320 / 2 / 2
Irrep combinations (i,i,i,j) (i,j,j,j) with indices: pos(A') ≤ i ≤ j ≤ pos(A'')
Subtotal: 0 / 0 / 2
Irrep combinations (i,i,j,j) with indices: pos(A') ≤ i ≤ j ≤ pos(A'')
..49.725. A'A'A''A''.
Subtotal: 49.725 / 1 / 1
Irrep combinations (i,i,j,k) (i,j,j,k) (i,j,k,k) with indices: pos(A') ≤ i ≤ j ≤ k ≤ pos(A'')
Subtotal: 0 / 0 / 0
Irrep combinations (i,j,k,l) with indices: pos(A') ≤ i ≤ j ≤ k ≤ l ≤ pos(A'')
Subtotal: 0 / 0 / 0
Total: 75.045 / 3 / 5


Calculate contributions to

A' A''
Show only nonzero contributions Show all contributions
Up to quartic force fieldUp to quintic force fieldUp to sextic force field






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