Vibrational Frequencies calculated at B3LYP/6-31+G**
| 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 |
3739 |
3605 |
132.33 |
|
|
|
| 2 |
A |
1230 |
1186 |
131.59 |
|
|
|
| 3 |
A |
1086 |
1047 |
78.89 |
|
|
|
| 4 |
A |
1042 |
1005 |
69.49 |
|
|
|
| 5 |
A |
705 |
679 |
156.29 |
|
|
|
| 6 |
A |
495 |
477 |
33.79 |
|
|
|
| 7 |
A |
398 |
383 |
9.06 |
|
|
|
| 8 |
A |
392 |
378 |
43.93 |
|
|
|
| 9 |
A |
275 |
265 |
96.14 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4680.0 cm
-1
Scaled (by 0.9642) Zero Point Vibrational Energy (zpe) 4512.5 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 B3LYP/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
1.166 |
|
|
|
| 2 |
O |
-0.555 |
|
|
|
| 3 |
O |
-0.512 |
|
|
|
| 4 |
O |
-0.484 |
|
|
|
| 5 |
H |
0.385 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.530 |
0.146 |
1.166 |
2.790 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.493 |
-0.560 |
-0.645 |
| y |
-0.560 |
-34.862 |
0.154 |
| z |
-0.645 |
0.154 |
-28.285 |
|
| Traceless |
| | x | y | z |
| x |
5.081 |
-0.560 |
-0.645 |
| y |
-0.560 |
-7.474 |
0.154 |
| z |
-0.645 |
0.154 |
2.393 |
|
| Polar |
| 3z2-r2 | 4.786 |
| x2-y2 | 8.370 |
| xy | -0.560 |
| xz | -0.645 |
| yz | 0.154 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.582 |
0.396 |
0.100 |
| y |
0.396 |
5.566 |
-0.057 |
| z |
0.100 |
-0.057 |
3.349 |
<r2> (average value of r
2) Å
2
| <r2> |
76.666 |
| (<r2>)1/2 |
8.756 |