Vibrational Frequencies calculated at HSEh1PBE/cc-pVDZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A |
3750 |
3607 |
126.65 |
|
|
|
| 2 |
A |
1246 |
1199 |
102.07 |
|
|
|
| 3 |
A |
1102 |
1060 |
83.40 |
|
|
|
| 4 |
A |
1060 |
1020 |
62.60 |
|
|
|
| 5 |
A |
756 |
727 |
136.19 |
|
|
|
| 6 |
A |
493 |
475 |
35.36 |
|
|
|
| 7 |
A |
401 |
385 |
12.63 |
|
|
|
| 8 |
A |
393 |
378 |
32.67 |
|
|
|
| 9 |
A |
250 |
240 |
93.27 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4725.8 cm
-1
Scaled (by 0.9619) Zero Point Vibrational Energy (zpe) 4545.7 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/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.889 |
|
|
|
| 2 |
O |
-0.314 |
|
|
|
| 3 |
O |
-0.403 |
|
|
|
| 4 |
O |
-0.370 |
|
|
|
| 5 |
H |
0.197 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.382 |
-0.156 |
0.973 |
2.578 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.108 |
-1.352 |
-0.788 |
| y |
-1.352 |
-33.173 |
0.236 |
| z |
-0.788 |
0.236 |
-27.110 |
|
| Traceless |
| | x | y | z |
| x |
4.033 |
-1.352 |
-0.788 |
| y |
-1.352 |
-6.564 |
0.236 |
| z |
-0.788 |
0.236 |
2.531 |
|
| Polar |
| 3z2-r2 | 5.063 |
| x2-y2 | 7.065 |
| xy | -1.352 |
| xz | -0.788 |
| yz | 0.236 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.750 |
0.381 |
0.046 |
| y |
0.381 |
4.340 |
-0.044 |
| z |
0.046 |
-0.044 |
2.302 |
<r2> (average value of r
2) Å
2
| <r2> |
76.000 |
| (<r2>)1/2 |
8.718 |