Vibrational Frequencies calculated at PBEPBE/6-31G*
| 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 |
3569 |
3518 |
83.26 |
|
|
|
| 2 |
A |
1225 |
1207 |
102.99 |
|
|
|
| 3 |
A |
1084 |
1068 |
88.59 |
|
|
|
| 4 |
A |
1020 |
1006 |
48.99 |
|
|
|
| 5 |
A |
677 |
668 |
119.97 |
|
|
|
| 6 |
A |
478 |
471 |
26.45 |
|
|
|
| 7 |
A |
376 |
370 |
12.09 |
|
|
|
| 8 |
A |
370 |
365 |
33.86 |
|
|
|
| 9 |
A |
236 |
233 |
90.27 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4517.0 cm
-1
Scaled (by 0.9857) Zero Point Vibrational Energy (zpe) 4452.4 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/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.959 |
|
|
|
| 2 |
O |
-0.581 |
|
|
|
| 3 |
O |
-0.421 |
|
|
|
| 4 |
O |
-0.386 |
|
|
|
| 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 |
| |
2.355 |
0.093 |
0.832 |
2.499 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.670 |
-0.726 |
-0.762 |
| y |
-0.726 |
-33.235 |
0.189 |
| z |
-0.762 |
0.189 |
-27.524 |
|
| Traceless |
| | x | y | z |
| x |
4.709 |
-0.726 |
-0.762 |
| y |
-0.726 |
-6.637 |
0.189 |
| z |
-0.762 |
0.189 |
1.928 |
|
| Polar |
| 3z2-r2 | 3.856 |
| x2-y2 | 7.564 |
| xy | -0.726 |
| xz | -0.762 |
| yz | 0.189 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.018 |
0.283 |
0.015 |
| y |
0.283 |
4.640 |
-0.027 |
| z |
0.015 |
-0.027 |
2.606 |
<r2> (average value of r
2) Å
2
| <r2> |
77.237 |
| (<r2>)1/2 |
8.788 |