Vibrational Frequencies calculated at PBEPBE/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 |
3578 |
3557 |
85.81 |
|
|
|
| 2 |
A |
1175 |
1168 |
89.86 |
|
|
|
| 3 |
A |
1039 |
1033 |
82.12 |
|
|
|
| 4 |
A |
992 |
986 |
46.90 |
|
|
|
| 5 |
A |
663 |
659 |
111.94 |
|
|
|
| 6 |
A |
456 |
454 |
25.48 |
|
|
|
| 7 |
A |
364 |
362 |
17.89 |
|
|
|
| 8 |
A |
360 |
358 |
22.82 |
|
|
|
| 9 |
A |
226 |
225 |
77.39 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4426.3 cm
-1
Scaled (by 0.9942) Zero Point Vibrational Energy (zpe) 4400.7 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 PBEPBE/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.784 |
|
|
|
| 2 |
O |
-0.285 |
|
|
|
| 3 |
O |
-0.357 |
|
|
|
| 4 |
O |
-0.328 |
|
|
|
| 5 |
H |
0.185 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.183 |
0.152 |
0.892 |
2.363 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.922 |
-0.458 |
-0.677 |
| y |
-0.458 |
-33.027 |
0.156 |
| z |
-0.677 |
0.156 |
-27.292 |
|
| Traceless |
| | x | y | z |
| x |
4.237 |
-0.458 |
-0.677 |
| y |
-0.458 |
-6.420 |
0.156 |
| z |
-0.677 |
0.156 |
2.183 |
|
| Polar |
| 3z2-r2 | 4.365 |
| x2-y2 | 7.105 |
| xy | -0.458 |
| xz | -0.677 |
| yz | 0.156 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.038 |
0.304 |
0.013 |
| y |
0.304 |
4.649 |
-0.019 |
| z |
0.013 |
-0.019 |
2.333 |
<r2> (average value of r
2) Å
2
| <r2> |
78.495 |
| (<r2>)1/2 |
8.860 |