Vibrational Frequencies calculated at LSDA/6-311G**
| 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 |
827 |
817 |
111.62 |
|
|
|
| 2 |
A1 |
545 |
538 |
3.81 |
|
|
|
| 3 |
A1 |
462 |
457 |
20.70 |
|
|
|
| 4 |
A1 |
190 |
187 |
0.72 |
|
|
|
| 5 |
A2 |
411 |
406 |
0.00 |
|
|
|
| 6 |
B1 |
801 |
791 |
168.59 |
|
|
|
| 7 |
B1 |
310 |
306 |
11.24 |
|
|
|
| 8 |
B2 |
748 |
739 |
514.67 |
|
|
|
| 9 |
B2 |
473 |
467 |
2.10 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2383.0 cm
-1
Scaled (by 0.9877) Zero Point Vibrational Energy (zpe) 2353.7 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 LSDA/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
1.144 |
|
|
|
| 2 |
F |
-0.336 |
|
|
|
| 3 |
F |
-0.336 |
|
|
|
| 4 |
F |
-0.236 |
|
|
|
| 5 |
F |
-0.236 |
|
|
|
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 |
1.044 |
1.044 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.055 |
0.000 |
0.000 |
| y |
0.000 |
-37.909 |
0.000 |
| z |
0.000 |
0.000 |
-30.981 |
|
| Traceless |
| | x | y | z |
| x |
2.390 |
0.000 |
0.000 |
| y |
0.000 |
-6.391 |
0.000 |
| z |
0.000 |
0.000 |
4.001 |
|
| Polar |
| 3z2-r2 | 8.002 |
| x2-y2 | 5.854 |
| 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 |
3.182 |
0.000 |
0.000 |
| y |
0.000 |
4.277 |
0.000 |
| z |
0.000 |
0.000 |
2.467 |
<r2> (average value of r
2) Å
2
| <r2> |
109.436 |
| (<r2>)1/2 |
10.461 |