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 |
A |
3808 |
3647 |
130.11 |
|
|
|
| 2 |
A |
1351 |
1294 |
129.58 |
|
|
|
| 3 |
A |
1130 |
1082 |
69.17 |
|
|
|
| 4 |
A |
1128 |
1080 |
80.27 |
|
|
|
| 5 |
A |
795 |
761 |
138.92 |
|
|
|
| 6 |
A |
535 |
512 |
27.61 |
|
|
|
| 7 |
A |
431 |
413 |
12.44 |
|
|
|
| 8 |
A |
424 |
406 |
32.05 |
|
|
|
| 9 |
A |
281 |
269 |
85.28 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4941.3 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 4732.3 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/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.448 |
|
|
|
| 2 |
O |
-0.338 |
|
|
|
| 3 |
O |
-0.249 |
|
|
|
| 4 |
O |
-0.214 |
|
|
|
| 5 |
H |
0.352 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.544 |
-0.287 |
0.807 |
2.684 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.242 |
-1.393 |
-0.675 |
| y |
-1.393 |
-32.206 |
0.217 |
| z |
-0.675 |
0.217 |
-27.132 |
|
| Traceless |
| | x | y | z |
| x |
4.427 |
-1.393 |
-0.675 |
| y |
-1.393 |
-6.019 |
0.217 |
| z |
-0.675 |
0.217 |
1.592 |
|
| Polar |
| 3z2-r2 | 3.184 |
| x2-y2 | 6.964 |
| xy | -1.393 |
| xz | -0.675 |
| yz | 0.217 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.750 |
0.224 |
0.029 |
| y |
0.224 |
4.387 |
-0.031 |
| z |
0.029 |
-0.031 |
2.929 |
<r2> (average value of r
2) Å
2
| <r2> |
72.880 |
| (<r2>)1/2 |
8.537 |