Vibrational Frequencies calculated at B1B95/CEP-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 |
A1 |
848 |
812 |
67.77 |
|
|
|
| 2 |
A1 |
402 |
385 |
67.48 |
|
|
|
| 3 |
A1 |
267 |
255 |
0.34 |
|
|
|
| 4 |
A1 |
131 |
125 |
0.13 |
|
|
|
| 5 |
A2 |
178 |
171 |
0.00 |
|
|
|
| 6 |
B1 |
429 |
411 |
173.46 |
|
|
|
| 7 |
B1 |
249 |
238 |
0.62 |
|
|
|
| 8 |
B2 |
970 |
929 |
68.36 |
|
|
|
| 9 |
B2 |
231 |
221 |
8.38 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1852.2 cm
-1
Scaled (by 0.9575) Zero Point Vibrational Energy (zpe) 1773.4 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 B1B95/CEP-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.657 |
|
|
|
| 2 |
O |
-0.307 |
|
|
|
| 3 |
O |
-0.307 |
|
|
|
| 4 |
Cl |
-0.021 |
|
|
|
| 5 |
Cl |
-0.021 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-1.231 |
1.231 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-47.090 |
0.000 |
0.000 |
| y |
0.000 |
-53.301 |
0.000 |
| z |
0.000 |
0.000 |
-50.288 |
|
| Traceless |
| | x | y | z |
| x |
4.704 |
0.000 |
0.000 |
| y |
0.000 |
-4.612 |
0.000 |
| z |
0.000 |
0.000 |
-0.092 |
|
| Polar |
| 3z2-r2 | -0.184 |
| x2-y2 | 6.211 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
11.995 |
0.000 |
0.000 |
| y |
0.000 |
5.820 |
0.000 |
| z |
0.000 |
0.000 |
9.194 |
<r2> (average value of r
2) Å
2
| <r2> |
0.000 |
| (<r2>)1/2 |
0.000 |