Vibrational Frequencies calculated at B1B95/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 |
1210 |
1160 |
150.67 |
|
|
|
| 2 |
A1 |
562 |
538 |
97.37 |
|
|
|
| 3 |
A1 |
397 |
381 |
0.41 |
|
|
|
| 4 |
A1 |
201 |
193 |
0.09 |
|
|
|
| 5 |
A2 |
266 |
255 |
0.00 |
|
|
|
| 6 |
B1 |
583 |
559 |
289.99 |
|
|
|
| 7 |
B1 |
376 |
361 |
1.69 |
|
|
|
| 8 |
B2 |
1446 |
1386 |
167.14 |
|
|
|
| 9 |
B2 |
350 |
335 |
3.65 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2695.2 cm
-1
Scaled (by 0.9585) Zero Point Vibrational Energy (zpe) 2583.4 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 B1B95/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
1.565 |
|
|
|
| 2 |
O |
-0.656 |
|
|
|
| 3 |
O |
-0.656 |
|
|
|
| 4 |
Cl |
-0.126 |
|
|
|
| 5 |
Cl |
-0.126 |
|
|
|
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 |
-1.800 |
1.800 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-44.218 |
0.000 |
0.000 |
| y |
0.000 |
-51.536 |
0.000 |
| z |
0.000 |
0.000 |
-48.574 |
|
| Traceless |
| | x | y | z |
| x |
5.837 |
0.000 |
0.000 |
| y |
0.000 |
-5.140 |
0.000 |
| z |
0.000 |
0.000 |
-0.697 |
|
| Polar |
| 3z2-r2 | -1.395 |
| x2-y2 | 7.318 |
| 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 |
9.906 |
0.000 |
0.000 |
| y |
0.000 |
7.197 |
0.000 |
| z |
0.000 |
0.000 |
8.395 |
<r2> (average value of r
2) Å
2
| <r2> |
185.519 |
| (<r2>)1/2 |
13.621 |