Vibrational Frequencies calculated at B3LYPultrafine/6-31+G**
| 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 |
1147 |
1104 |
158.38 |
|
|
|
| 2 |
A1 |
530 |
511 |
106.38 |
|
|
|
| 3 |
A1 |
363 |
349 |
1.82 |
|
|
|
| 4 |
A1 |
191 |
184 |
0.02 |
|
|
|
| 5 |
A2 |
255 |
246 |
0.00 |
|
|
|
| 6 |
B1 |
552 |
531 |
300.40 |
|
|
|
| 7 |
B1 |
348 |
335 |
4.47 |
|
|
|
| 8 |
B2 |
1375 |
1324 |
186.19 |
|
|
|
| 9 |
B2 |
336 |
323 |
6.86 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2548.1 cm
-1
Scaled (by 0.9627) Zero Point Vibrational Energy (zpe) 2453.1 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 B3LYPultrafine/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.535 |
|
|
|
| 2 |
O |
-0.341 |
|
|
|
| 3 |
O |
-0.341 |
|
|
|
| 4 |
Cl |
0.073 |
|
|
|
| 5 |
Cl |
0.073 |
|
|
|
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 |
-1.553 |
1.553 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-46.042 |
0.000 |
0.000 |
| y |
0.000 |
-52.833 |
-0.004 |
| z |
0.000 |
-0.004 |
-49.913 |
|
| Traceless |
| | x | y | z |
| x |
5.331 |
0.000 |
0.000 |
| y |
0.000 |
-4.855 |
-0.004 |
| z |
0.000 |
-0.004 |
-0.476 |
|
| Polar |
| 3z2-r2 | -0.952 |
| x2-y2 | 6.791 |
| 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 |
9.597 |
0.000 |
0.000 |
| y |
0.000 |
6.443 |
-0.004 |
| z |
0.000 |
-0.004 |
7.859 |
<r2> (average value of r
2) Å
2
| <r2> |
194.175 |
| (<r2>)1/2 |
13.935 |