Vibrational Frequencies calculated at B97D3/aug-cc-pVTZ
| 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 |
3658 |
3602 |
99.25 |
|
|
|
| 2 |
A |
1232 |
1213 |
131.99 |
|
|
|
| 3 |
A |
1086 |
1070 |
76.15 |
|
|
|
| 4 |
A |
1030 |
1015 |
58.59 |
|
|
|
| 5 |
A |
671 |
661 |
137.01 |
|
|
|
| 6 |
A |
488 |
480 |
19.19 |
|
|
|
| 7 |
A |
393 |
387 |
8.81 |
|
|
|
| 8 |
A |
391 |
385 |
31.89 |
|
|
|
| 9 |
A |
279 |
275 |
71.05 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4613.9 cm
-1
Scaled (by 0.9847) Zero Point Vibrational Energy (zpe) 4543.3 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 B97D3/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
1.408 |
|
|
|
| 2 |
O |
-0.385 |
|
|
|
| 3 |
O |
-0.624 |
|
|
|
| 4 |
O |
-0.595 |
|
|
|
| 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 |
| |
-2.337 |
0.273 |
-0.948 |
2.536 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.073 |
-0.174 |
-0.588 |
| y |
-0.174 |
-33.538 |
-0.111 |
| z |
-0.588 |
-0.111 |
-28.024 |
|
| Traceless |
| | x | y | z |
| x |
4.708 |
-0.174 |
-0.588 |
| y |
-0.174 |
-6.489 |
-0.111 |
| z |
-0.588 |
-0.111 |
1.782 |
|
| Polar |
| 3z2-r2 | 3.564 |
| x2-y2 | 7.465 |
| xy | -0.174 |
| xz | -0.588 |
| yz | -0.111 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.069 |
-0.211 |
0.041 |
| y |
-0.211 |
5.928 |
0.021 |
| z |
0.041 |
0.021 |
3.964 |
<r2> (average value of r
2) Å
2
| <r2> |
76.206 |
| (<r2>)1/2 |
8.730 |