Vibrational Frequencies calculated at B3PW91/cc-pVTZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A |
3771 |
3626 |
127.91 |
|
|
|
| 2 |
A |
1307 |
1257 |
137.58 |
|
|
|
| 3 |
A |
1112 |
1070 |
83.55 |
|
|
|
| 4 |
A |
1101 |
1059 |
64.69 |
|
|
|
| 5 |
A |
763 |
734 |
151.25 |
|
|
|
| 6 |
A |
522 |
502 |
28.18 |
|
|
|
| 7 |
A |
422 |
406 |
10.63 |
|
|
|
| 8 |
A |
413 |
397 |
30.54 |
|
|
|
| 9 |
A |
269 |
259 |
89.69 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4839.9 cm
-1
Scaled (by 0.9616) Zero Point Vibrational Energy (zpe) 4654.1 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-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.807 |
|
|
|
| 2 |
O |
-0.286 |
|
|
|
| 3 |
O |
-0.385 |
|
|
|
| 4 |
O |
-0.357 |
|
|
|
| 5 |
H |
0.221 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.550 |
-0.103 |
0.957 |
2.725 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.691 |
-0.952 |
-0.657 |
| y |
-0.952 |
-33.226 |
0.179 |
| z |
-0.657 |
0.179 |
-27.430 |
|
| Traceless |
| | x | y | z |
| x |
4.637 |
-0.952 |
-0.657 |
| y |
-0.952 |
-6.666 |
0.179 |
| z |
-0.657 |
0.179 |
2.029 |
|
| Polar |
| 3z2-r2 | 4.058 |
| x2-y2 | 7.535 |
| xy | -0.952 |
| xz | -0.657 |
| yz | 0.179 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.033 |
0.309 |
0.056 |
| y |
0.309 |
4.808 |
-0.034 |
| z |
0.056 |
-0.034 |
2.949 |
<r2> (average value of r
2) Å
2
| <r2> |
74.168 |
| (<r2>)1/2 |
8.612 |