Vibrational Frequencies calculated at M06-2X/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 |
A1 |
1281 |
1217 |
183.64 |
|
|
|
| 2 |
A1 |
890 |
846 |
110.10 |
|
|
|
| 3 |
A1 |
538 |
512 |
35.03 |
|
|
|
| 4 |
A1 |
366 |
347 |
0.00 |
|
|
|
| 5 |
A2 |
360 |
342 |
0.00 |
|
|
|
| 6 |
B1 |
937 |
891 |
240.94 |
|
|
|
| 7 |
B1 |
522 |
496 |
30.35 |
|
|
|
| 8 |
B2 |
1507 |
1432 |
287.32 |
|
|
|
| 9 |
B2 |
523 |
497 |
36.41 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3461.3 cm
-1
Scaled (by 0.9504) Zero Point Vibrational Energy (zpe) 3289.6 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 M06-2X/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
1.417 |
|
|
|
| 2 |
O |
-0.438 |
|
|
|
| 3 |
O |
-0.438 |
|
|
|
| 4 |
F |
-0.270 |
|
|
|
| 5 |
F |
-0.270 |
|
|
|
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 |
-1.047 |
1.047 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.341 |
0.000 |
0.000 |
| y |
0.000 |
-35.870 |
0.000 |
| z |
0.000 |
0.000 |
-33.271 |
|
| Traceless |
| | x | y | z |
| x |
3.230 |
0.000 |
0.000 |
| y |
0.000 |
-3.564 |
0.000 |
| z |
0.000 |
0.000 |
0.334 |
|
| Polar |
| 3z2-r2 | 0.669 |
| x2-y2 | 4.529 |
| 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 |
2.809 |
0.000 |
0.000 |
| y |
0.000 |
3.653 |
0.000 |
| z |
0.000 |
0.000 |
3.096 |
<r2> (average value of r
2) Å
2
| <r2> |
95.727 |
| (<r2>)1/2 |
9.784 |