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 |
3652 |
3607 |
132.04 |
|
|
|
| 2 |
A |
1265 |
1250 |
131.05 |
|
|
|
| 3 |
A |
1062 |
1049 |
69.61 |
|
|
|
| 4 |
A |
1008 |
996 |
81.24 |
|
|
|
| 5 |
A |
716 |
707 |
145.59 |
|
|
|
| 6 |
A |
497 |
491 |
33.10 |
|
|
|
| 7 |
A |
394 |
389 |
28.96 |
|
|
|
| 8 |
A |
391 |
386 |
30.37 |
|
|
|
| 9 |
A |
258 |
254 |
99.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4621.1 cm
-1
Scaled (by 0.9877) Zero Point Vibrational Energy (zpe) 4564.2 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 |
0.890 |
|
|
|
| 2 |
O |
-0.425 |
|
|
|
| 3 |
O |
-0.408 |
|
|
|
| 4 |
O |
-0.367 |
|
|
|
| 5 |
H |
0.310 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.579 |
-0.093 |
1.051 |
2.786 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.265 |
-1.402 |
-0.602 |
| y |
-1.402 |
-34.197 |
0.223 |
| z |
-0.602 |
0.223 |
-27.766 |
|
| Traceless |
| | x | y | z |
| x |
4.717 |
-1.402 |
-0.602 |
| y |
-1.402 |
-7.182 |
0.223 |
| z |
-0.602 |
0.223 |
2.466 |
|
| Polar |
| 3z2-r2 | 4.931 |
| x2-y2 | 7.932 |
| xy | -1.402 |
| xz | -0.602 |
| yz | 0.223 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.007 |
0.287 |
0.015 |
| y |
0.287 |
4.559 |
-0.024 |
| z |
0.015 |
-0.024 |
2.566 |
<r2> (average value of r
2) Å
2
| <r2> |
75.458 |
| (<r2>)1/2 |
8.687 |