Vibrational Frequencies calculated at HSEh1PBE/6-31G(2df,p)
| 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 |
1293 |
1238 |
146.87 |
|
|
|
| 2 |
A1 |
854 |
818 |
102.10 |
|
|
|
| 3 |
A1 |
542 |
519 |
24.31 |
|
|
|
| 4 |
A1 |
375 |
359 |
0.08 |
|
|
|
| 5 |
A2 |
374 |
359 |
0.00 |
|
|
|
| 6 |
B1 |
901 |
863 |
206.41 |
|
|
|
| 7 |
B1 |
530 |
508 |
19.70 |
|
|
|
| 8 |
B2 |
1531 |
1467 |
238.47 |
|
|
|
| 9 |
B2 |
532 |
509 |
27.40 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3466.0 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 3319.4 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/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.535 |
|
|
|
| 2 |
O |
-0.230 |
|
|
|
| 3 |
O |
-0.230 |
|
|
|
| 4 |
F |
-0.037 |
|
|
|
| 5 |
F |
-0.037 |
|
|
|
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 |
-1.170 |
1.170 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-30.608 |
0.000 |
0.000 |
| y |
0.000 |
-34.828 |
0.000 |
| z |
0.000 |
0.000 |
-32.424 |
|
| Traceless |
| | x | y | z |
| x |
3.018 |
0.000 |
0.000 |
| y |
0.000 |
-3.312 |
0.000 |
| z |
0.000 |
0.000 |
0.294 |
|
| Polar |
| 3z2-r2 | 0.589 |
| x2-y2 | 4.220 |
| 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 |
3.227 |
0.000 |
0.000 |
| y |
0.000 |
3.897 |
0.000 |
| z |
0.000 |
0.000 |
3.457 |
<r2> (average value of r
2) Å
2
| <r2> |
93.619 |
| (<r2>)1/2 |
9.676 |