Vibrational Frequencies calculated at HF/6-31G(2df,p)
| 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 |
4101 |
3714 |
199.62 |
|
|
|
| 2 |
A |
1487 |
1347 |
213.22 |
|
|
|
| 3 |
A |
1258 |
1140 |
104.75 |
|
|
|
| 4 |
A |
1235 |
1119 |
107.36 |
|
|
|
| 5 |
A |
936 |
848 |
171.80 |
|
|
|
| 6 |
A |
614 |
556 |
55.71 |
|
|
|
| 7 |
A |
503 |
455 |
28.66 |
|
|
|
| 8 |
A |
476 |
431 |
27.69 |
|
|
|
| 9 |
A |
325 |
294 |
108.31 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5468.4 cm
-1
Scaled (by 0.9055) Zero Point Vibrational Energy (zpe) 4951.7 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 HF/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.739 |
|
|
|
| 2 |
O |
-0.423 |
|
|
|
| 3 |
O |
-0.370 |
|
|
|
| 4 |
O |
-0.332 |
|
|
|
| 5 |
H |
0.386 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.881 |
-0.384 |
1.044 |
3.089 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.541 |
-1.610 |
-0.959 |
| y |
-1.610 |
-33.121 |
0.265 |
| z |
-0.959 |
0.265 |
-26.929 |
|
| Traceless |
| | x | y | z |
| x |
4.484 |
-1.610 |
-0.959 |
| y |
-1.610 |
-6.886 |
0.265 |
| z |
-0.959 |
0.265 |
2.402 |
|
| Polar |
| 3z2-r2 | 4.804 |
| x2-y2 | 7.580 |
| xy | -1.610 |
| xz | -0.959 |
| yz | 0.265 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.157 |
0.277 |
0.064 |
| y |
0.277 |
3.909 |
-0.045 |
| z |
0.064 |
-0.045 |
2.766 |
<r2> (average value of r
2) Å
2
| <r2> |
70.495 |
| (<r2>)1/2 |
8.396 |