Vibrational Frequencies calculated at mPW1PW91/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 |
3803 |
3647 |
134.07 |
|
|
|
| 2 |
A |
1327 |
1273 |
142.29 |
|
|
|
| 3 |
A |
1122 |
1076 |
101.81 |
|
|
|
| 4 |
A |
1119 |
1073 |
51.24 |
|
|
|
| 5 |
A |
786 |
754 |
153.53 |
|
|
|
| 6 |
A |
530 |
508 |
29.87 |
|
|
|
| 7 |
A |
429 |
412 |
12.38 |
|
|
|
| 8 |
A |
419 |
402 |
30.42 |
|
|
|
| 9 |
A |
274 |
263 |
90.83 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4904.5 cm
-1
Scaled (by 0.9592) Zero Point Vibrational Energy (zpe) 4704.4 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 mPW1PW91/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.810 |
|
|
|
| 2 |
O |
-0.282 |
|
|
|
| 3 |
O |
-0.388 |
|
|
|
| 4 |
O |
-0.359 |
|
|
|
| 5 |
H |
0.220 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.577 |
-0.189 |
0.955 |
2.755 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.720 |
-1.170 |
-0.678 |
| y |
-1.170 |
-33.151 |
0.196 |
| z |
-0.678 |
0.196 |
-27.391 |
|
| Traceless |
| | x | y | z |
| x |
4.551 |
-1.170 |
-0.678 |
| y |
-1.170 |
-6.596 |
0.196 |
| z |
-0.678 |
0.196 |
2.044 |
|
| Polar |
| 3z2-r2 | 4.089 |
| x2-y2 | 7.431 |
| xy | -1.170 |
| xz | -0.678 |
| yz | 0.196 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.973 |
0.314 |
0.057 |
| y |
0.314 |
4.725 |
-0.038 |
| z |
0.057 |
-0.038 |
2.934 |
<r2> (average value of r
2) Å
2
| <r2> |
73.691 |
| (<r2>)1/2 |
8.584 |