Vibrational Frequencies calculated at B3LYPultrafine/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 |
1176 |
1137 |
144.91 |
|
|
|
| 2 |
A1 |
546 |
527 |
98.16 |
|
|
|
| 3 |
A1 |
373 |
360 |
2.02 |
|
|
|
| 4 |
A1 |
194 |
188 |
0.06 |
|
|
|
| 5 |
A2 |
260 |
251 |
0.00 |
|
|
|
| 6 |
B1 |
559 |
541 |
294.03 |
|
|
|
| 7 |
B1 |
354 |
342 |
5.27 |
|
|
|
| 8 |
B2 |
1409 |
1362 |
162.05 |
|
|
|
| 9 |
B2 |
341 |
330 |
4.66 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2605.8 cm
-1
Scaled (by 0.9667) Zero Point Vibrational Energy (zpe) 2519.0 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 B3LYPultrafine/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.860 |
|
|
|
| 2 |
O |
-0.347 |
|
|
|
| 3 |
O |
-0.347 |
|
|
|
| 4 |
Cl |
-0.083 |
|
|
|
| 5 |
Cl |
-0.083 |
|
|
|
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 |
-1.581 |
1.581 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-44.885 |
0.000 |
0.000 |
| y |
0.000 |
-51.697 |
-0.004 |
| z |
0.000 |
-0.004 |
-48.779 |
|
| Traceless |
| | x | y | z |
| x |
5.353 |
0.000 |
0.000 |
| y |
0.000 |
-4.865 |
-0.004 |
| z |
0.000 |
-0.004 |
-0.488 |
|
| Polar |
| 3z2-r2 | -0.976 |
| x2-y2 | 6.812 |
| xy | 0.000 |
| xz | 0.000 |
| yz | -0.004 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
9.159 |
0.000 |
0.000 |
| y |
0.000 |
5.954 |
-0.004 |
| z |
0.000 |
-0.004 |
7.455 |
<r2> (average value of r
2) Å
2
| <r2> |
190.949 |
| (<r2>)1/2 |
13.818 |