Vibrational Frequencies calculated at B3PW91/STO-3G
| 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 |
940 |
832 |
50.80 |
|
|
|
| 2 |
A1 |
678 |
600 |
20.49 |
|
|
|
| 3 |
A1 |
287 |
254 |
14.50 |
|
|
|
| 4 |
A1 |
208 |
184 |
0.46 |
|
|
|
| 5 |
A2 |
210 |
186 |
0.00 |
|
|
|
| 6 |
B1 |
721 |
638 |
67.02 |
|
|
|
| 7 |
B1 |
272 |
241 |
14.04 |
|
|
|
| 8 |
B2 |
1071 |
948 |
32.36 |
|
|
|
| 9 |
B2 |
306 |
271 |
12.48 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2346.0 cm
-1
Scaled (by 0.885) Zero Point Vibrational Energy (zpe) 2076.2 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/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.873 |
|
|
|
| 2 |
O |
-0.297 |
|
|
|
| 3 |
O |
-0.297 |
|
|
|
| 4 |
F |
-0.139 |
|
|
|
| 5 |
F |
-0.139 |
|
|
|
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 |
-0.512 |
0.512 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-28.340 |
0.000 |
0.000 |
| y |
0.000 |
-32.299 |
0.000 |
| z |
0.000 |
0.000 |
-29.920 |
|
| Traceless |
| | x | y | z |
| x |
2.769 |
0.000 |
0.000 |
| y |
0.000 |
-3.169 |
0.000 |
| z |
0.000 |
0.000 |
0.400 |
|
| Polar |
| 3z2-r2 | 0.800 |
| x2-y2 | 3.959 |
| 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 |
2.179 |
0.000 |
0.000 |
| y |
0.000 |
3.209 |
0.000 |
| z |
0.000 |
0.000 |
2.672 |
<r2> (average value of r
2) Å
2
| <r2> |
113.672 |
| (<r2>)1/2 |
10.662 |