Vibrational Frequencies calculated at LSDA/6-311G*
| 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 |
3610 |
3551 |
103.38 |
|
|
|
| 2 |
A |
1267 |
1247 |
136.98 |
|
|
|
| 3 |
A |
1062 |
1045 |
50.93 |
|
|
|
| 4 |
A |
1047 |
1030 |
103.95 |
|
|
|
| 5 |
A |
716 |
704 |
151.98 |
|
|
|
| 6 |
A |
498 |
489 |
33.60 |
|
|
|
| 7 |
A |
399 |
392 |
50.36 |
|
|
|
| 8 |
A |
391 |
385 |
21.20 |
|
|
|
| 9 |
A |
265 |
260 |
110.38 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4627.0 cm
-1
Scaled (by 0.9837) Zero Point Vibrational Energy (zpe) 4551.6 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 LSDA/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.909 |
|
|
|
| 2 |
O |
-0.582 |
|
|
|
| 3 |
O |
-0.408 |
|
|
|
| 4 |
O |
-0.367 |
|
|
|
| 5 |
H |
0.448 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.693 |
0.060 |
1.062 |
2.896 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.765 |
-1.143 |
-0.617 |
| y |
-1.143 |
-34.515 |
0.194 |
| z |
-0.617 |
0.194 |
-27.828 |
|
| Traceless |
| | x | y | z |
| x |
5.406 |
-1.143 |
-0.617 |
| y |
-1.143 |
-7.718 |
0.194 |
| z |
-0.617 |
0.194 |
2.312 |
|
| Polar |
| 3z2-r2 | 4.624 |
| x2-y2 | 8.749 |
| xy | -1.143 |
| xz | -0.617 |
| yz | 0.194 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.976 |
0.289 |
0.011 |
| y |
0.289 |
4.567 |
-0.019 |
| z |
0.011 |
-0.019 |
2.531 |
<r2> (average value of r
2) Å
2
| <r2> |
75.522 |
| (<r2>)1/2 |
8.690 |