Vibrational Frequencies calculated at LSDA/6-311G**
| 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 |
1230 |
1215 |
154.65 |
|
|
|
| 2 |
A1 |
784 |
774 |
126.83 |
|
|
|
| 3 |
A1 |
495 |
489 |
24.20 |
|
|
|
| 4 |
A1 |
338 |
334 |
0.01 |
|
|
|
| 5 |
A2 |
343 |
339 |
0.00 |
|
|
|
| 6 |
B1 |
831 |
821 |
239.79 |
|
|
|
| 7 |
B1 |
484 |
478 |
18.74 |
|
|
|
| 8 |
B2 |
1480 |
1462 |
251.62 |
|
|
|
| 9 |
B2 |
491 |
485 |
32.85 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3237.7 cm
-1
Scaled (by 0.9877) Zero Point Vibrational Energy (zpe) 3197.8 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 LSDA/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
1.167 |
|
|
|
| 2 |
O |
-0.352 |
|
|
|
| 3 |
O |
-0.352 |
|
|
|
| 4 |
F |
-0.231 |
|
|
|
| 5 |
F |
-0.231 |
|
|
|
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 |
-0.622 |
0.622 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.475 |
0.000 |
0.000 |
| y |
0.000 |
-36.206 |
0.000 |
| z |
0.000 |
0.000 |
-34.031 |
|
| Traceless |
| | x | y | z |
| x |
2.643 |
0.000 |
0.000 |
| y |
0.000 |
-2.952 |
0.000 |
| z |
0.000 |
0.000 |
0.309 |
|
| Polar |
| 3z2-r2 | 0.619 |
| x2-y2 | 3.730 |
| 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 |
2.918 |
0.000 |
0.000 |
| y |
0.000 |
3.931 |
0.000 |
| z |
0.000 |
0.000 |
3.252 |
<r2> (average value of r
2) Å
2
| <r2> |
97.357 |
| (<r2>)1/2 |
9.867 |