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 |
A |
3494 |
3354 |
73.33 |
|
|
|
| 2 |
A |
1263 |
1212 |
72.64 |
|
|
|
| 3 |
A |
1088 |
1044 |
5.14 |
|
|
|
| 4 |
A |
1068 |
1025 |
102.35 |
|
|
|
| 5 |
A |
768 |
737 |
161.07 |
|
|
|
| 6 |
A |
500 |
480 |
40.89 |
|
|
|
| 7 |
A |
418 |
401 |
23.54 |
|
|
|
| 8 |
A |
385 |
370 |
30.76 |
|
|
|
| 9 |
A |
195 |
188 |
157.29 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4589.5 cm
-1
Scaled (by 0.9599) Zero Point Vibrational Energy (zpe) 4405.4 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/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
1.036 |
|
|
|
| 2 |
O |
-0.583 |
|
|
|
| 3 |
O |
-0.451 |
|
|
|
| 4 |
O |
-0.403 |
|
|
|
| 5 |
H |
0.401 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.528 |
-0.034 |
0.447 |
2.567 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.857 |
-1.311 |
-1.954 |
| y |
-1.311 |
-33.596 |
0.493 |
| z |
-1.954 |
0.493 |
-26.354 |
|
| Traceless |
| | x | y | z |
| x |
4.118 |
-1.311 |
-1.954 |
| y |
-1.311 |
-7.490 |
0.493 |
| z |
-1.954 |
0.493 |
3.372 |
|
| Polar |
| 3z2-r2 | 6.744 |
| x2-y2 | 7.738 |
| xy | -1.311 |
| xz | -1.954 |
| yz | 0.493 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.226 |
0.356 |
-0.058 |
| y |
0.356 |
3.673 |
-0.064 |
| z |
-0.058 |
-0.064 |
2.044 |
<r2> (average value of r
2) Å
2
| <r2> |
74.956 |
| (<r2>)1/2 |
8.658 |