Vibrational Frequencies calculated at B3PW91/cc-pVDZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
3159 |
3049 |
29.83 |
|
|
|
| 2 |
A1 |
1853 |
1788 |
373.67 |
|
|
|
| 3 |
A1 |
1340 |
1293 |
2.00 |
|
|
|
| 4 |
A1 |
868 |
837 |
14.36 |
|
|
|
| 5 |
B1 |
684 |
660 |
84.88 |
|
|
|
| 6 |
B1 |
421 |
407 |
2.75 |
|
|
|
| 7 |
B2 |
3257 |
3143 |
7.20 |
|
|
|
| 8 |
B2 |
907 |
875 |
0.19 |
|
|
|
| 9 |
B2 |
357 |
344 |
1.93 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6423.0 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 6198.2 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.127 |
|
|
|
| 2 |
C |
0.004 |
|
|
|
| 3 |
S |
-0.072 |
|
|
|
| 4 |
H |
0.098 |
|
|
|
| 5 |
H |
0.098 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-1.156 |
1.156 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-27.017 |
0.000 |
0.000 |
| y |
0.000 |
-23.092 |
0.000 |
| z |
0.000 |
0.000 |
-21.158 |
|
| Traceless |
| | x | y | z |
| x |
-4.892 |
0.000 |
0.000 |
| y |
0.000 |
0.996 |
0.000 |
| z |
0.000 |
0.000 |
3.896 |
|
| Polar |
| 3z2-r2 | 7.793 |
| x2-y2 | -3.926 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.465 |
0.000 |
0.000 |
| y |
0.000 |
3.215 |
0.000 |
| z |
0.000 |
0.000 |
10.404 |
<r2> (average value of r
2) Å
2
| <r2> |
67.257 |
| (<r2>)1/2 |
8.201 |