Vibrational Frequencies calculated at B3PW91/6-31G
| 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 |
3548 |
3398 |
72.89 |
|
|
|
| 2 |
A |
1111 |
1064 |
47.83 |
|
|
|
| 3 |
A |
813 |
779 |
9.01 |
|
|
|
| 4 |
A |
639 |
612 |
32.99 |
|
|
|
| 5 |
A |
622 |
596 |
74.59 |
|
|
|
| 6 |
A |
347 |
332 |
65.22 |
|
|
|
| 7 |
A |
294 |
281 |
38.38 |
|
|
|
| 8 |
A |
248 |
237 |
4.50 |
|
|
|
| 9 |
A |
198 |
190 |
163.33 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3909.5 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 3744.2 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 B3PW91/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
1.166 |
|
|
|
| 2 |
O |
-0.630 |
|
|
|
| 3 |
O |
-0.524 |
|
|
|
| 4 |
O |
-0.424 |
|
|
|
| 5 |
H |
0.413 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.780 |
-0.049 |
0.351 |
1.815 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-29.039 |
-1.300 |
-2.947 |
| y |
-1.300 |
-36.237 |
1.085 |
| z |
-2.947 |
1.085 |
-27.030 |
|
| Traceless |
| | x | y | z |
| x |
2.594 |
-1.300 |
-2.947 |
| y |
-1.300 |
-8.202 |
1.085 |
| z |
-2.947 |
1.085 |
5.608 |
|
| Polar |
| 3z2-r2 | 11.217 |
| x2-y2 | 7.197 |
| xy | -1.300 |
| xz | -2.947 |
| yz | 1.085 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.690 |
1.106 |
0.068 |
| y |
1.106 |
6.050 |
-0.074 |
| z |
0.068 |
-0.074 |
2.512 |
<r2> (average value of r
2) Å
2
| <r2> |
87.909 |
| (<r2>)1/2 |
9.376 |