Vibrational Frequencies calculated at mPW1PW91/aug-cc-pVTZ
| 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 |
1269 |
1215 |
161.42 |
|
|
|
| 2 |
A1 |
838 |
802 |
122.64 |
|
|
|
| 3 |
A1 |
535 |
512 |
25.46 |
|
|
|
| 4 |
A1 |
370 |
354 |
0.03 |
|
|
|
| 5 |
A2 |
368 |
352 |
0.00 |
|
|
|
| 6 |
B1 |
872 |
836 |
236.86 |
|
|
|
| 7 |
B1 |
521 |
500 |
20.08 |
|
|
|
| 8 |
B2 |
1501 |
1438 |
272.15 |
|
|
|
| 9 |
B2 |
525 |
503 |
30.53 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3398.9 cm
-1
Scaled (by 0.9581) Zero Point Vibrational Energy (zpe) 3256.5 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 mPW1PW91/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
2.077 |
|
|
|
| 2 |
O |
-0.645 |
|
|
|
| 3 |
O |
-0.645 |
|
|
|
| 4 |
F |
-0.394 |
|
|
|
| 5 |
F |
-0.394 |
|
|
|
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 |
-1.044 |
1.044 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.633 |
0.000 |
0.000 |
| y |
0.000 |
-35.823 |
0.000 |
| z |
0.000 |
0.000 |
-33.423 |
|
| Traceless |
| | x | y | z |
| x |
2.990 |
0.000 |
0.000 |
| y |
0.000 |
-3.296 |
0.000 |
| z |
0.000 |
0.000 |
0.306 |
|
| Polar |
| 3z2-r2 | 0.611 |
| x2-y2 | 4.190 |
| 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 |
3.884 |
0.000 |
0.000 |
| y |
0.000 |
4.611 |
0.000 |
| z |
0.000 |
0.000 |
4.144 |
<r2> (average value of r
2) Å
2
| <r2> |
95.085 |
| (<r2>)1/2 |
9.751 |