Vibrational Frequencies calculated at HF/CEP-31G*
| 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 |
4035 |
3623 |
150.07 |
|
|
|
| 2 |
A |
1307 |
1174 |
178.74 |
|
|
|
| 3 |
A |
1212 |
1088 |
84.35 |
|
|
|
| 4 |
A |
905 |
813 |
243.91 |
|
|
|
| 5 |
A |
757 |
679 |
67.34 |
|
|
|
| 6 |
A |
495 |
445 |
68.56 |
|
|
|
| 7 |
A |
475 |
427 |
129.83 |
|
|
|
| 8 |
A |
362 |
325 |
27.18 |
|
|
|
| 9 |
A |
275 |
247 |
45.78 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4911.1 cm
-1
Scaled (by 0.898) Zero Point Vibrational Energy (zpe) 4410.1 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/CEP-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.782 |
|
|
|
| 2 |
O |
-0.567 |
|
|
|
| 3 |
O |
-0.517 |
|
|
|
| 4 |
O |
-0.169 |
|
|
|
| 5 |
H |
0.471 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.170 |
-1.083 |
-0.038 |
1.594 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-27.863 |
-1.004 |
-3.348 |
| y |
-1.004 |
-34.268 |
-1.296 |
| z |
-3.348 |
-1.296 |
-25.471 |
|
| Traceless |
| | x | y | z |
| x |
2.007 |
-1.004 |
-3.348 |
| y |
-1.004 |
-7.601 |
-1.296 |
| z |
-3.348 |
-1.296 |
5.594 |
|
| Polar |
| 3z2-r2 | 11.188 |
| x2-y2 | 6.405 |
| xy | -1.004 |
| xz | -3.348 |
| yz | -1.296 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.981 |
-0.133 |
-0.034 |
| y |
-0.133 |
3.978 |
0.121 |
| z |
-0.034 |
0.121 |
2.779 |
<r2> (average value of r
2) Å
2
| <r2> |
60.047 |
| (<r2>)1/2 |
7.749 |