Vibrational Frequencies calculated at HF/6-31G*
| 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 |
1376 |
1236 |
227.56 |
|
|
|
| 2 |
A1 |
959 |
862 |
129.27 |
|
|
|
| 3 |
A1 |
597 |
537 |
52.38 |
|
|
|
| 4 |
A1 |
408 |
366 |
0.05 |
|
|
|
| 5 |
A2 |
402 |
361 |
0.00 |
|
|
|
| 6 |
B1 |
1005 |
903 |
290.46 |
|
|
|
| 7 |
B1 |
585 |
526 |
47.66 |
|
|
|
| 8 |
B2 |
1614 |
1451 |
393.20 |
|
|
|
| 9 |
B2 |
579 |
521 |
49.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3763.0 cm
-1
Scaled (by 0.8985) Zero Point Vibrational Energy (zpe) 3381.0 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 HF/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
1.763 |
|
|
|
| 2 |
O |
-0.542 |
|
|
|
| 3 |
O |
-0.542 |
|
|
|
| 4 |
F |
-0.340 |
|
|
|
| 5 |
F |
-0.340 |
|
|
|
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 |
-1.303 |
1.303 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.384 |
0.000 |
0.000 |
| y |
0.000 |
-36.723 |
-0.020 |
| z |
0.000 |
-0.020 |
-33.659 |
|
| Traceless |
| | x | y | z |
| x |
3.807 |
0.000 |
0.000 |
| y |
0.000 |
-4.201 |
-0.020 |
| z |
0.000 |
-0.020 |
0.394 |
|
| Polar |
| 3z2-r2 | 0.789 |
| x2-y2 | 5.339 |
| xy | 0.000 |
| xz | 0.000 |
| yz | -0.020 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.540 |
0.000 |
0.000 |
| y |
0.000 |
3.205 |
0.003 |
| z |
0.000 |
0.003 |
2.758 |
<r2> (average value of r
2) Å
2
| <r2> |
93.186 |
| (<r2>)1/2 |
9.653 |