Vibrational Frequencies calculated at HF/CEP-121G*
| 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 |
4019 |
3631 |
135.87 |
|
|
|
| 2 |
A |
1307 |
1181 |
187.05 |
|
|
|
| 3 |
A |
1217 |
1099 |
83.51 |
|
|
|
| 4 |
A |
903 |
816 |
242.15 |
|
|
|
| 5 |
A |
753 |
681 |
67.08 |
|
|
|
| 6 |
A |
493 |
446 |
69.94 |
|
|
|
| 7 |
A |
472 |
426 |
119.69 |
|
|
|
| 8 |
A |
359 |
324 |
26.10 |
|
|
|
| 9 |
A |
273 |
247 |
41.85 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4897.8 cm
-1
Scaled (by 0.9034) Zero Point Vibrational Energy (zpe) 4424.7 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 HF/CEP-121G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.939 |
|
|
|
| 2 |
O |
-0.636 |
|
|
|
| 3 |
O |
-0.582 |
|
|
|
| 4 |
O |
-0.203 |
|
|
|
| 5 |
H |
0.483 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.138 |
-1.052 |
-0.103 |
1.553 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-27.843 |
-0.976 |
-3.327 |
| y |
-0.976 |
-34.098 |
-1.256 |
| z |
-3.327 |
-1.256 |
-25.343 |
|
| Traceless |
| | x | y | z |
| x |
1.877 |
-0.976 |
-3.327 |
| y |
-0.976 |
-7.505 |
-1.256 |
| z |
-3.327 |
-1.256 |
5.627 |
|
| Polar |
| 3z2-r2 | 11.255 |
| x2-y2 | 6.255 |
| xy | -0.976 |
| xz | -3.327 |
| yz | -1.256 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.139 |
-0.139 |
-0.037 |
| y |
-0.139 |
4.127 |
0.104 |
| z |
-0.037 |
0.104 |
2.989 |
<r2> (average value of r
2) Å
2
| <r2> |
59.937 |
| (<r2>)1/2 |
7.742 |