Vibrational Frequencies calculated at HSEh1PBE/3-21G
| 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 |
1073 |
1034 |
102.02 |
|
|
|
| 2 |
A1 |
753 |
726 |
52.96 |
|
|
|
| 3 |
A1 |
413 |
397 |
27.89 |
|
|
|
| 4 |
A1 |
271 |
261 |
0.44 |
|
|
|
| 5 |
A2 |
279 |
269 |
0.00 |
|
|
|
| 6 |
B1 |
837 |
806 |
134.10 |
|
|
|
| 7 |
B1 |
375 |
362 |
29.99 |
|
|
|
| 8 |
B2 |
1237 |
1192 |
85.53 |
|
|
|
| 9 |
B2 |
401 |
386 |
31.61 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2819.8 cm
-1
Scaled (by 0.9633) Zero Point Vibrational Energy (zpe) 2716.3 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 HSEh1PBE/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
1.631 |
|
|
|
| 2 |
O |
-0.521 |
|
|
|
| 3 |
O |
-0.521 |
|
|
|
| 4 |
F |
-0.295 |
|
|
|
| 5 |
F |
-0.295 |
|
|
|
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 |
-0.516 |
0.516 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.707 |
0.000 |
0.000 |
| y |
0.000 |
-37.089 |
0.000 |
| z |
0.000 |
0.000 |
-34.672 |
|
| Traceless |
| | x | y | z |
| x |
3.173 |
0.000 |
0.000 |
| y |
0.000 |
-3.399 |
0.000 |
| z |
0.000 |
0.000 |
0.226 |
|
| Polar |
| 3z2-r2 | 0.452 |
| x2-y2 | 4.382 |
| 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 |
2.719 |
0.000 |
0.000 |
| y |
0.000 |
3.991 |
0.000 |
| z |
0.000 |
0.000 |
3.330 |
<r2> (average value of r
2) Å
2
| <r2> |
108.060 |
| (<r2>)1/2 |
10.395 |