Vibrational Frequencies calculated at LSDA/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 |
3639 |
3599 |
131.63 |
|
|
|
| 2 |
A |
1295 |
1281 |
133.63 |
|
|
|
| 3 |
A |
1087 |
1075 |
75.26 |
|
|
|
| 4 |
A |
1052 |
1041 |
71.01 |
|
|
|
| 5 |
A |
750 |
741 |
142.73 |
|
|
|
| 6 |
A |
506 |
501 |
25.83 |
|
|
|
| 7 |
A |
404 |
400 |
32.73 |
|
|
|
| 8 |
A |
402 |
397 |
14.09 |
|
|
|
| 9 |
A |
263 |
261 |
82.04 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4699.2 cm
-1
Scaled (by 0.9891) Zero Point Vibrational Energy (zpe) 4648.0 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 LSDA/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.694 |
|
|
|
| 2 |
O |
-0.263 |
|
|
|
| 3 |
O |
-0.342 |
|
|
|
| 4 |
O |
-0.313 |
|
|
|
| 5 |
H |
0.225 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.501 |
-0.304 |
0.846 |
2.657 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.997 |
-1.551 |
-0.698 |
| y |
-1.551 |
-33.048 |
0.248 |
| z |
-0.698 |
0.248 |
-27.741 |
|
| Traceless |
| | x | y | z |
| x |
4.397 |
-1.551 |
-0.698 |
| y |
-1.551 |
-6.179 |
0.248 |
| z |
-0.698 |
0.248 |
1.782 |
|
| Polar |
| 3z2-r2 | 3.563 |
| x2-y2 | 7.050 |
| xy | -1.551 |
| xz | -0.698 |
| yz | 0.248 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.249 |
0.243 |
0.023 |
| y |
0.243 |
4.840 |
-0.025 |
| z |
0.023 |
-0.025 |
2.997 |
<r2> (average value of r
2) Å
2
| <r2> |
74.390 |
| (<r2>)1/2 |
8.625 |