Vibrational Frequencies calculated at wB97X-D/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 |
3567 |
3380 |
87.31 |
|
|
|
| 2 |
A |
1269 |
1203 |
76.00 |
|
|
|
| 3 |
A |
1097 |
1040 |
3.75 |
|
|
|
| 4 |
A |
1078 |
1022 |
108.07 |
|
|
|
| 5 |
A |
785 |
744 |
174.46 |
|
|
|
| 6 |
A |
510 |
484 |
44.92 |
|
|
|
| 7 |
A |
428 |
406 |
22.92 |
|
|
|
| 8 |
A |
395 |
374 |
29.66 |
|
|
|
| 9 |
A |
181 |
172 |
168.59 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4655.0 cm
-1
Scaled (by 0.9478) Zero Point Vibrational Energy (zpe) 4412.0 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 wB97X-D/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
1.057 |
|
|
|
| 2 |
O |
-0.595 |
|
|
|
| 3 |
O |
-0.458 |
|
|
|
| 4 |
O |
-0.412 |
|
|
|
| 5 |
H |
0.408 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.633 |
0.037 |
-0.567 |
2.694 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.541 |
1.169 |
-1.856 |
| y |
1.169 |
-33.766 |
-0.416 |
| z |
-1.856 |
-0.416 |
-26.297 |
|
| Traceless |
| | x | y | z |
| x |
4.490 |
1.169 |
-1.856 |
| y |
1.169 |
-7.847 |
-0.416 |
| z |
-1.856 |
-0.416 |
3.357 |
|
| Polar |
| 3z2-r2 | 6.713 |
| x2-y2 | 8.225 |
| xy | 1.169 |
| xz | -1.856 |
| yz | -0.416 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.115 |
-0.379 |
-0.024 |
| y |
-0.379 |
3.650 |
0.065 |
| z |
-0.024 |
0.065 |
2.012 |
<r2> (average value of r
2) Å
2
| <r2> |
74.553 |
| (<r2>)1/2 |
8.634 |