Vibrational Frequencies calculated at mPW1PW91/STO-3G
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
944 |
830 |
54.49 |
|
|
|
| 2 |
A1 |
692 |
608 |
18.29 |
|
|
|
| 3 |
A1 |
293 |
257 |
15.76 |
|
|
|
| 4 |
A1 |
213 |
187 |
0.64 |
|
|
|
| 5 |
A2 |
214 |
188 |
0.00 |
|
|
|
| 6 |
B1 |
738 |
649 |
66.84 |
|
|
|
| 7 |
B1 |
275 |
242 |
15.47 |
|
|
|
| 8 |
B2 |
1073 |
943 |
33.43 |
|
|
|
| 9 |
B2 |
311 |
273 |
13.15 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2376.1 cm
-1
Scaled (by 0.8789) Zero Point Vibrational Energy (zpe) 2088.3 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/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.896 |
|
|
|
| 2 |
O |
-0.305 |
|
|
|
| 3 |
O |
-0.305 |
|
|
|
| 4 |
F |
-0.143 |
|
|
|
| 5 |
F |
-0.143 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-0.564 |
0.564 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-28.339 |
0.000 |
0.000 |
| y |
0.000 |
-32.462 |
0.000 |
| z |
0.000 |
0.000 |
-30.000 |
|
| Traceless |
| | x | y | z |
| x |
2.892 |
0.000 |
0.000 |
| y |
0.000 |
-3.292 |
0.000 |
| z |
0.000 |
0.000 |
0.400 |
|
| Polar |
| 3z2-r2 | 0.801 |
| x2-y2 | 4.123 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.142 |
0.000 |
0.000 |
| y |
0.000 |
3.181 |
0.000 |
| z |
0.000 |
0.000 |
2.643 |
<r2> (average value of r
2) Å
2
| <r2> |
112.815 |
| (<r2>)1/2 |
10.621 |