Vibrational Frequencies calculated at mPW1PW91/6-31G**
| 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 |
3814 |
3629 |
128.28 |
|
|
|
| 2 |
A |
1300 |
1237 |
120.62 |
|
|
|
| 3 |
A |
1120 |
1066 |
93.13 |
|
|
|
| 4 |
A |
1096 |
1043 |
66.88 |
|
|
|
| 5 |
A |
775 |
737 |
148.72 |
|
|
|
| 6 |
A |
519 |
494 |
38.35 |
|
|
|
| 7 |
A |
414 |
394 |
13.70 |
|
|
|
| 8 |
A |
404 |
384 |
35.84 |
|
|
|
| 9 |
A |
258 |
245 |
106.28 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4849.5 cm
-1
Scaled (by 0.9515) Zero Point Vibrational Energy (zpe) 4614.3 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 mPW1PW91/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
1.082 |
|
|
|
| 2 |
O |
-0.543 |
|
|
|
| 3 |
O |
-0.474 |
|
|
|
| 4 |
O |
-0.435 |
|
|
|
| 5 |
H |
0.370 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.544 |
-0.233 |
0.958 |
2.728 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.878 |
-1.622 |
-0.824 |
| y |
-1.622 |
-33.235 |
0.267 |
| z |
-0.824 |
0.267 |
-27.234 |
|
| Traceless |
| | x | y | z |
| x |
4.357 |
-1.622 |
-0.824 |
| y |
-1.622 |
-6.679 |
0.267 |
| z |
-0.824 |
0.267 |
2.322 |
|
| Polar |
| 3z2-r2 | 4.644 |
| x2-y2 | 7.357 |
| xy | -1.622 |
| xz | -0.824 |
| yz | 0.267 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.700 |
0.353 |
0.054 |
| y |
0.353 |
4.300 |
-0.053 |
| z |
0.054 |
-0.053 |
2.557 |
<r2> (average value of r
2) Å
2
| <r2> |
74.699 |
| (<r2>)1/2 |
8.643 |