Vibrational Frequencies calculated at HF/cc-pVDZ
| 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 |
4021 |
3651 |
165.37 |
|
|
|
| 2 |
A |
1294 |
1175 |
171.92 |
|
|
|
| 3 |
A |
1203 |
1092 |
50.95 |
|
|
|
| 4 |
A |
900 |
818 |
227.69 |
|
|
|
| 5 |
A |
746 |
678 |
69.18 |
|
|
|
| 6 |
A |
490 |
445 |
62.99 |
|
|
|
| 7 |
A |
474 |
430 |
119.05 |
|
|
|
| 8 |
A |
361 |
328 |
18.85 |
|
|
|
| 9 |
A |
293 |
266 |
39.26 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4890.8 cm
-1
Scaled (by 0.908) Zero Point Vibrational Energy (zpe) 4440.8 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/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
1.136 |
|
|
|
| 2 |
O |
-0.429 |
|
|
|
| 3 |
O |
-0.612 |
|
|
|
| 4 |
O |
-0.296 |
|
|
|
| 5 |
H |
0.202 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.099 |
-1.019 |
-0.277 |
1.525 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-28.532 |
-0.826 |
-3.099 |
| y |
-0.826 |
-34.455 |
-1.153 |
| z |
-3.099 |
-1.153 |
-25.750 |
|
| Traceless |
| | x | y | z |
| x |
1.571 |
-0.826 |
-3.099 |
| y |
-0.826 |
-7.314 |
-1.153 |
| z |
-3.099 |
-1.153 |
5.743 |
|
| Polar |
| 3z2-r2 | 11.486 |
| x2-y2 | 5.923 |
| xy | -0.826 |
| xz | -3.099 |
| yz | -1.153 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.731 |
-0.116 |
-0.074 |
| y |
-0.116 |
3.669 |
0.089 |
| z |
-0.074 |
0.089 |
2.515 |
<r2> (average value of r
2) Å
2
| <r2> |
74.621 |
| (<r2>)1/2 |
8.638 |