Vibrational Frequencies calculated at HF/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 |
3783 |
3414 |
118.66 |
|
|
|
| 2 |
A |
1321 |
1193 |
199.86 |
|
|
|
| 3 |
A |
1186 |
1071 |
15.37 |
|
|
|
| 4 |
A |
941 |
849 |
265.79 |
|
|
|
| 5 |
A |
773 |
698 |
74.34 |
|
|
|
| 6 |
A |
524 |
473 |
144.97 |
|
|
|
| 7 |
A |
504 |
455 |
107.96 |
|
|
|
| 8 |
A |
379 |
342 |
11.66 |
|
|
|
| 9 |
A |
323 |
292 |
72.36 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4867.0 cm
-1
Scaled (by 0.9026) Zero Point Vibrational Energy (zpe) 4393.0 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 HF/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
1.272 |
|
|
|
| 2 |
O |
-0.719 |
|
|
|
| 3 |
O |
-0.631 |
|
|
|
| 4 |
O |
-0.351 |
|
|
|
| 5 |
H |
0.429 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.366 |
-0.846 |
0.047 |
1.607 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-28.318 |
-1.067 |
-3.897 |
| y |
-1.067 |
-34.443 |
-1.448 |
| z |
-3.897 |
-1.448 |
-25.177 |
|
| Traceless |
| | x | y | z |
| x |
1.492 |
-1.067 |
-3.897 |
| y |
-1.067 |
-7.696 |
-1.448 |
| z |
-3.897 |
-1.448 |
6.204 |
|
| Polar |
| 3z2-r2 | 12.408 |
| x2-y2 | 6.125 |
| xy | -1.067 |
| xz | -3.897 |
| yz | -1.448 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.135 |
-0.101 |
-0.164 |
| y |
-0.101 |
3.144 |
0.108 |
| z |
-0.164 |
0.108 |
2.218 |
<r2> (average value of r
2) Å
2
| <r2> |
74.026 |
| (<r2>)1/2 |
8.604 |