Vibrational Frequencies calculated at wB97X-D/3-21G*
| 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 |
1214 |
1150 |
141.34 |
|
|
|
| 2 |
A1 |
561 |
532 |
119.62 |
|
|
|
| 3 |
A1 |
395 |
375 |
2.11 |
|
|
|
| 4 |
A1 |
213 |
202 |
0.08 |
|
|
|
| 5 |
A2 |
269 |
255 |
0.00 |
|
|
|
| 6 |
B1 |
576 |
546 |
338.72 |
|
|
|
| 7 |
B1 |
368 |
348 |
4.46 |
|
|
|
| 8 |
B2 |
1482 |
1405 |
148.99 |
|
|
|
| 9 |
B2 |
356 |
337 |
10.82 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2716.5 cm
-1
Scaled (by 0.9478) Zero Point Vibrational Energy (zpe) 2574.7 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 wB97X-D/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.951 |
|
|
|
| 2 |
O |
-0.371 |
|
|
|
| 3 |
O |
-0.371 |
|
|
|
| 4 |
Cl |
-0.105 |
|
|
|
| 5 |
Cl |
-0.105 |
|
|
|
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 |
-1.223 |
1.223 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-46.399 |
0.000 |
0.000 |
| y |
0.000 |
-51.892 |
0.000 |
| z |
0.000 |
0.000 |
-49.220 |
|
| Traceless |
| | x | y | z |
| x |
4.157 |
0.000 |
0.000 |
| y |
0.000 |
-4.083 |
0.000 |
| z |
0.000 |
0.000 |
-0.074 |
|
| Polar |
| 3z2-r2 | -0.148 |
| x2-y2 | 5.493 |
| 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 |
7.445 |
0.000 |
0.000 |
| y |
0.000 |
4.387 |
0.000 |
| z |
0.000 |
0.000 |
5.885 |
<r2> (average value of r
2) Å
2
| <r2> |
187.633 |
| (<r2>)1/2 |
13.698 |