Vibrational Frequencies calculated at mPW1PW91/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 |
3759 |
3602 |
127.46 |
|
|
|
| 2 |
A |
1248 |
1196 |
102.70 |
|
|
|
| 3 |
A |
1103 |
1057 |
83.33 |
|
|
|
| 4 |
A |
1063 |
1018 |
62.82 |
|
|
|
| 5 |
A |
757 |
726 |
137.50 |
|
|
|
| 6 |
A |
495 |
474 |
35.93 |
|
|
|
| 7 |
A |
402 |
385 |
12.65 |
|
|
|
| 8 |
A |
395 |
378 |
32.96 |
|
|
|
| 9 |
A |
253 |
242 |
93.49 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4736.5 cm
-1
Scaled (by 0.9583) Zero Point Vibrational Energy (zpe) 4539.0 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 mPW1PW91/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.899 |
|
|
|
| 2 |
O |
-0.316 |
|
|
|
| 3 |
O |
-0.407 |
|
|
|
| 4 |
O |
-0.374 |
|
|
|
| 5 |
H |
0.198 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.391 |
-0.151 |
0.987 |
2.591 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.070 |
-1.337 |
-0.781 |
| y |
-1.337 |
-33.174 |
0.231 |
| z |
-0.781 |
0.231 |
-27.064 |
|
| Traceless |
| | x | y | z |
| x |
4.050 |
-1.337 |
-0.781 |
| y |
-1.337 |
-6.607 |
0.231 |
| z |
-0.781 |
0.231 |
2.558 |
|
| Polar |
| 3z2-r2 | 5.115 |
| x2-y2 | 7.105 |
| xy | -1.337 |
| xz | -0.781 |
| yz | 0.231 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.731 |
0.387 |
0.048 |
| y |
0.387 |
4.336 |
-0.044 |
| z |
0.048 |
-0.044 |
2.297 |
<r2> (average value of r
2) Å
2
| <r2> |
75.905 |
| (<r2>)1/2 |
8.712 |