Vibrational Frequencies calculated at B3PW91/6-31G
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 |
779 |
746 |
75.93 |
|
|
|
2 |
A1 |
537 |
514 |
1.64 |
|
|
|
3 |
A1 |
291 |
279 |
32.41 |
|
|
|
4 |
B1 |
285 |
273 |
0.00 |
|
|
|
5 |
B2 |
517 |
495 |
0.00 |
|
|
|
6 |
B2 |
103 |
99 |
0.00 |
|
|
|
7 |
E |
709 |
679 |
214.11 |
|
|
|
7 |
E |
709 |
679 |
214.11 |
|
|
|
8 |
E |
310 |
296 |
4.15 |
|
|
|
8 |
E |
310 |
296 |
4.15 |
|
|
|
9 |
E |
203 |
194 |
0.80 |
|
|
|
9 |
E |
203 |
194 |
0.80 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2477.5 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 2372.7 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 B3PW91/6-31G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
S |
1.585 |
|
|
|
2 |
F |
-0.293 |
|
|
|
3 |
F |
-0.323 |
|
|
|
4 |
F |
-0.323 |
|
|
|
5 |
F |
-0.323 |
|
|
|
6 |
F |
-0.323 |
|
|
|
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 |
0.843 |
0.843 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-41.719 |
0.000 |
0.000 |
y |
0.000 |
-41.719 |
0.000 |
z |
0.000 |
0.000 |
-36.207 |
|
Traceless |
| x | y | z |
x |
-2.756 |
0.000 |
0.000 |
y |
0.000 |
-2.756 |
0.000 |
z |
0.000 |
0.000 |
5.513 |
|
Polar |
3z2-r2 | 11.025 |
x2-y2 | 0.000 |
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 |
5.272 |
0.000 |
0.000 |
y |
0.000 |
5.272 |
0.000 |
z |
0.000 |
0.000 |
2.940 |
<r2> (average value of r
2) Å
2
<r2> |
162.874 |
(<r2>)1/2 |
12.762 |