Vibrational Frequencies calculated at LSDA/6-31+G**
| 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 |
3638 |
3583 |
138.19 |
|
|
|
| 2 |
A |
1258 |
1240 |
149.15 |
|
|
|
| 3 |
A |
1058 |
1042 |
80.47 |
|
|
|
| 4 |
A |
1020 |
1005 |
76.94 |
|
|
|
| 5 |
A |
724 |
713 |
149.97 |
|
|
|
| 6 |
A |
488 |
481 |
29.97 |
|
|
|
| 7 |
A |
390 |
384 |
52.60 |
|
|
|
| 8 |
A |
385 |
379 |
10.31 |
|
|
|
| 9 |
A |
270 |
266 |
86.34 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4616.2 cm
-1
Scaled (by 0.985) Zero Point Vibrational Energy (zpe) 4546.9 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/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.995 |
|
|
|
| 2 |
O |
-0.518 |
|
|
|
| 3 |
O |
-0.451 |
|
|
|
| 4 |
O |
-0.424 |
|
|
|
| 5 |
H |
0.397 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.570 |
-0.172 |
1.037 |
2.776 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.427 |
-1.531 |
-0.560 |
| y |
-1.531 |
-34.316 |
0.209 |
| z |
-0.560 |
0.209 |
-28.502 |
|
| Traceless |
| | x | y | z |
| x |
4.982 |
-1.531 |
-0.560 |
| y |
-1.531 |
-6.851 |
0.209 |
| z |
-0.560 |
0.209 |
1.869 |
|
| Polar |
| 3z2-r2 | 3.738 |
| x2-y2 | 7.889 |
| xy | -1.531 |
| xz | -0.560 |
| yz | 0.209 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.750 |
0.323 |
0.068 |
| y |
0.323 |
5.506 |
-0.054 |
| z |
0.068 |
-0.054 |
3.441 |
<r2> (average value of r
2) Å
2
| <r2> |
76.229 |
| (<r2>)1/2 |
8.731 |