Vibrational Frequencies calculated at B97D3/6-311G**
| 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 |
3673 |
3621 |
94.03 |
|
|
|
| 2 |
A |
1202 |
1185 |
112.70 |
|
|
|
| 3 |
A |
1054 |
1039 |
79.68 |
|
|
|
| 4 |
A |
1008 |
994 |
56.47 |
|
|
|
| 5 |
A |
640 |
631 |
133.69 |
|
|
|
| 6 |
A |
479 |
472 |
29.03 |
|
|
|
| 7 |
A |
380 |
374 |
8.43 |
|
|
|
| 8 |
A |
375 |
370 |
37.50 |
|
|
|
| 9 |
A |
255 |
252 |
95.27 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4533.5 cm
-1
Scaled (by 0.9857) Zero Point Vibrational Energy (zpe) 4468.7 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 B97D3/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.935 |
|
|
|
| 2 |
O |
-0.429 |
|
|
|
| 3 |
O |
-0.418 |
|
|
|
| 4 |
O |
-0.381 |
|
|
|
| 5 |
H |
0.293 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.359 |
0.470 |
-1.115 |
2.651 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.124 |
-0.387 |
-0.574 |
| y |
-0.387 |
-34.176 |
-0.112 |
| z |
-0.574 |
-0.112 |
-27.503 |
|
| Traceless |
| | x | y | z |
| x |
4.716 |
-0.387 |
-0.574 |
| y |
-0.387 |
-7.363 |
-0.112 |
| z |
-0.574 |
-0.112 |
2.647 |
|
| Polar |
| 3z2-r2 | 5.295 |
| x2-y2 | 8.053 |
| xy | -0.387 |
| xz | -0.574 |
| yz | -0.112 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.055 |
-0.318 |
0.030 |
| y |
-0.318 |
4.876 |
0.017 |
| z |
0.030 |
0.017 |
2.574 |
<r2> (average value of r
2) Å
2
| <r2> |
77.069 |
| (<r2>)1/2 |
8.779 |