Vibrational Frequencies calculated at B97D3/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 |
1139 |
1123 |
126.10 |
|
|
|
| 2 |
A1 |
519 |
512 |
88.42 |
|
|
|
| 3 |
A1 |
347 |
342 |
4.51 |
|
|
|
| 4 |
A1 |
186 |
184 |
0.08 |
|
|
|
| 5 |
A2 |
252 |
249 |
0.00 |
|
|
|
| 6 |
B1 |
527 |
519 |
267.71 |
|
|
|
| 7 |
B1 |
331 |
326 |
11.76 |
|
|
|
| 8 |
B2 |
1371 |
1352 |
140.21 |
|
|
|
| 9 |
B2 |
329 |
325 |
3.99 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2500.6 cm
-1
Scaled (by 0.986) Zero Point Vibrational Energy (zpe) 2465.6 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 B97D3/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.805 |
|
|
|
| 2 |
O |
-0.314 |
|
|
|
| 3 |
O |
-0.314 |
|
|
|
| 4 |
Cl |
-0.088 |
|
|
|
| 5 |
Cl |
-0.088 |
|
|
|
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 |
-1.253 |
1.253 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-44.901 |
0.000 |
0.000 |
| y |
0.000 |
-50.845 |
0.000 |
| z |
0.000 |
0.000 |
-48.132 |
|
| Traceless |
| | x | y | z |
| x |
4.587 |
0.000 |
0.000 |
| y |
0.000 |
-4.328 |
0.000 |
| z |
0.000 |
0.000 |
-0.259 |
|
| Polar |
| 3z2-r2 | -0.519 |
| x2-y2 | 5.943 |
| 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 |
9.445 |
0.000 |
0.000 |
| y |
0.000 |
6.151 |
0.000 |
| z |
0.000 |
0.000 |
7.712 |
<r2> (average value of r
2) Å
2
| <r2> |
193.181 |
| (<r2>)1/2 |
13.899 |