Vibrational Frequencies calculated at PBEPBEultrafine/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 |
1118 |
1099 |
121.28 |
|
|
|
| 2 |
A1 |
510 |
502 |
94.72 |
|
|
|
| 3 |
A1 |
350 |
344 |
3.40 |
|
|
|
| 4 |
A1 |
183 |
180 |
0.01 |
|
|
|
| 5 |
A2 |
243 |
239 |
0.00 |
|
|
|
| 6 |
B1 |
526 |
518 |
275.56 |
|
|
|
| 7 |
B1 |
331 |
325 |
6.20 |
|
|
|
| 8 |
B2 |
1360 |
1337 |
135.45 |
|
|
|
| 9 |
B2 |
324 |
319 |
6.82 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2471.9 cm
-1
Scaled (by 0.9835) Zero Point Vibrational Energy (zpe) 2431.1 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 PBEPBEultrafine/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.801 |
|
|
|
| 2 |
O |
-0.347 |
|
|
|
| 3 |
O |
-0.347 |
|
|
|
| 4 |
Cl |
-0.053 |
|
|
|
| 5 |
Cl |
-0.053 |
|
|
|
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 |
-0.934 |
0.934 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-46.441 |
0.000 |
0.000 |
| y |
0.000 |
-51.137 |
-0.003 |
| z |
0.000 |
-0.003 |
-48.789 |
|
| Traceless |
| | x | y | z |
| x |
3.522 |
0.000 |
0.000 |
| y |
0.000 |
-3.522 |
-0.003 |
| z |
0.000 |
-0.003 |
0.000 |
|
| Polar |
| 3z2-r2 | 0.001 |
| x2-y2 | 4.696 |
| xy | 0.000 |
| xz | 0.000 |
| yz | -0.003 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
8.827 |
0.000 |
0.000 |
| y |
0.000 |
5.300 |
-0.005 |
| z |
0.000 |
-0.005 |
6.983 |
<r2> (average value of r
2) Å
2
| <r2> |
195.980 |
| (<r2>)1/2 |
13.999 |