Vibrational Frequencies calculated at mPW1PW91/6-311G*
| 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 |
3789 |
3616 |
105.65 |
|
|
|
| 2 |
A |
1294 |
1235 |
140.60 |
|
|
|
| 3 |
A |
1126 |
1075 |
74.66 |
|
|
|
| 4 |
A |
1089 |
1040 |
85.94 |
|
|
|
| 5 |
A |
753 |
718 |
164.74 |
|
|
|
| 6 |
A |
520 |
496 |
40.94 |
|
|
|
| 7 |
A |
419 |
400 |
12.80 |
|
|
|
| 8 |
A |
413 |
394 |
50.17 |
|
|
|
| 9 |
A |
277 |
265 |
122.44 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4839.9 cm
-1
Scaled (by 0.9544) Zero Point Vibrational Energy (zpe) 4619.2 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 mPW1PW91/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
1.030 |
|
|
|
| 2 |
O |
-0.613 |
|
|
|
| 3 |
O |
-0.456 |
|
|
|
| 4 |
O |
-0.413 |
|
|
|
| 5 |
H |
0.451 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.715 |
0.129 |
1.182 |
2.964 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.757 |
-0.862 |
-0.641 |
| y |
-0.862 |
-34.613 |
0.169 |
| z |
-0.641 |
0.169 |
-27.487 |
|
| Traceless |
| | x | y | z |
| x |
5.293 |
-0.862 |
-0.641 |
| y |
-0.862 |
-7.990 |
0.169 |
| z |
-0.641 |
0.169 |
2.698 |
|
| Polar |
| 3z2-r2 | 5.395 |
| x2-y2 | 8.856 |
| xy | -0.862 |
| xz | -0.641 |
| yz | 0.169 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.717 |
0.391 |
0.059 |
| y |
0.391 |
4.487 |
-0.038 |
| z |
0.059 |
-0.038 |
2.480 |
<r2> (average value of r
2) Å
2
| <r2> |
74.750 |
| (<r2>)1/2 |
8.646 |