Vibrational Frequencies calculated at B3LYP/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 |
A |
3423 |
3293 |
51.75 |
|
|
|
| 2 |
A |
1209 |
1163 |
59.10 |
|
|
|
| 3 |
A |
1076 |
1035 |
35.68 |
|
|
|
| 4 |
A |
1031 |
992 |
58.95 |
|
|
|
| 5 |
A |
716 |
689 |
144.96 |
|
|
|
| 6 |
A |
485 |
466 |
38.04 |
|
|
|
| 7 |
A |
405 |
389 |
19.84 |
|
|
|
| 8 |
A |
370 |
356 |
26.80 |
|
|
|
| 9 |
A |
186 |
179 |
149.54 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4449.8 cm
-1
Scaled (by 0.962) Zero Point Vibrational Energy (zpe) 4280.7 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 B3LYP/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
1.015 |
|
|
|
| 2 |
O |
-0.563 |
|
|
|
| 3 |
O |
-0.441 |
|
|
|
| 4 |
O |
-0.394 |
|
|
|
| 5 |
H |
0.383 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.370 |
0.086 |
0.382 |
2.402 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.055 |
-0.922 |
-2.056 |
| y |
-0.922 |
-33.593 |
0.442 |
| z |
-2.056 |
0.442 |
-26.324 |
|
| Traceless |
| | x | y | z |
| x |
3.904 |
-0.922 |
-2.056 |
| y |
-0.922 |
-7.403 |
0.442 |
| z |
-2.056 |
0.442 |
3.500 |
|
| Polar |
| 3z2-r2 | 7.000 |
| x2-y2 | 7.538 |
| xy | -0.922 |
| xz | -2.056 |
| yz | 0.442 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.338 |
0.356 |
-0.089 |
| y |
0.356 |
3.799 |
-0.067 |
| z |
-0.089 |
-0.067 |
2.059 |
<r2> (average value of r
2) Å
2
| <r2> |
75.928 |
| (<r2>)1/2 |
8.714 |