Vibrational Frequencies calculated at HSEh1PBE/TZVP
| 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 |
1232 |
1183 |
174.80 |
|
|
|
| 2 |
A1 |
805 |
772 |
143.82 |
|
|
|
| 3 |
A1 |
507 |
486 |
28.99 |
|
|
|
| 4 |
A1 |
352 |
338 |
0.07 |
|
|
|
| 5 |
A2 |
354 |
340 |
0.00 |
|
|
|
| 6 |
B1 |
837 |
804 |
266.47 |
|
|
|
| 7 |
B1 |
501 |
481 |
21.09 |
|
|
|
| 8 |
B2 |
1478 |
1419 |
300.70 |
|
|
|
| 9 |
B2 |
507 |
487 |
37.51 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3285.6 cm
-1
Scaled (by 0.9601) Zero Point Vibrational Energy (zpe) 3154.5 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 HSEh1PBE/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.918 |
|
|
|
| 2 |
O |
-0.284 |
|
|
|
| 3 |
O |
-0.284 |
|
|
|
| 4 |
F |
-0.175 |
|
|
|
| 5 |
F |
-0.175 |
|
|
|
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 |
-0.676 |
0.676 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.386 |
0.000 |
0.000 |
| y |
0.000 |
-36.399 |
0.000 |
| z |
0.000 |
0.000 |
-34.022 |
|
| Traceless |
| | x | y | z |
| x |
2.824 |
0.000 |
0.000 |
| y |
0.000 |
-3.194 |
0.000 |
| z |
0.000 |
0.000 |
0.370 |
|
| Polar |
| 3z2-r2 | 0.740 |
| x2-y2 | 4.013 |
| 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 |
3.110 |
0.000 |
0.000 |
| y |
0.000 |
4.173 |
0.000 |
| z |
0.000 |
0.000 |
3.458 |
<r2> (average value of r
2) Å
2
| <r2> |
97.641 |
| (<r2>)1/2 |
9.881 |