Vibrational Frequencies calculated at HF/aug-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 |
A1 |
1313 |
1196 |
218.00 |
|
|
|
| 2 |
A1 |
639 |
582 |
121.94 |
|
|
|
| 3 |
A1 |
454 |
413 |
0.05 |
|
|
|
| 4 |
A1 |
231 |
211 |
0.08 |
|
|
|
| 5 |
A2 |
303 |
276 |
0.00 |
|
|
|
| 6 |
B1 |
665 |
606 |
356.30 |
|
|
|
| 7 |
B1 |
433 |
394 |
0.01 |
|
|
|
| 8 |
B2 |
1556 |
1416 |
244.16 |
|
|
|
| 9 |
B2 |
395 |
359 |
5.38 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2994.5 cm
-1
Scaled (by 0.9104) Zero Point Vibrational Energy (zpe) 2726.2 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 HF/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
1.936 |
|
|
|
| 2 |
O |
-0.781 |
|
|
|
| 3 |
O |
-0.781 |
|
|
|
| 4 |
Cl |
-0.187 |
|
|
|
| 5 |
Cl |
-0.187 |
|
|
|
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 |
-2.344 |
2.344 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-43.985 |
0.000 |
0.000 |
| y |
0.000 |
-52.802 |
0.000 |
| z |
0.000 |
0.000 |
-49.489 |
|
| Traceless |
| | x | y | z |
| x |
7.161 |
0.000 |
0.000 |
| y |
0.000 |
-6.065 |
0.000 |
| z |
0.000 |
0.000 |
-1.096 |
|
| Polar |
| 3z2-r2 | -2.191 |
| x2-y2 | 8.817 |
| 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 |
9.021 |
0.000 |
0.000 |
| y |
0.000 |
6.479 |
0.000 |
| z |
0.000 |
0.000 |
7.540 |
<r2> (average value of r
2) Å
2
| <r2> |
181.828 |
| (<r2>)1/2 |
13.484 |