Vibrational Frequencies calculated at B3PW91/cc-pVDZ
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 |
876 |
846 |
147.16 |
|
|
|
2 |
A1 |
623 |
602 |
5.54 |
|
|
|
3 |
A1 |
488 |
471 |
31.21 |
|
|
|
4 |
B1 |
411 |
396 |
0.00 |
|
|
|
5 |
B2 |
596 |
575 |
0.00 |
|
|
|
6 |
B2 |
212 |
205 |
0.00 |
|
|
|
7 |
E |
841 |
812 |
418.35 |
|
|
|
7 |
E |
841 |
812 |
418.35 |
|
|
|
8 |
E |
466 |
450 |
3.18 |
|
|
|
8 |
E |
466 |
450 |
3.18 |
|
|
|
9 |
E |
321 |
310 |
0.06 |
|
|
|
9 |
E |
321 |
310 |
0.06 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3230.6 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 3117.5 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/cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
S |
1.307 |
|
|
|
2 |
F |
-0.227 |
|
|
|
3 |
F |
-0.270 |
|
|
|
4 |
F |
-0.270 |
|
|
|
5 |
F |
-0.270 |
|
|
|
6 |
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 |
0.505 |
0.505 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-39.065 |
0.000 |
0.000 |
y |
0.000 |
-39.065 |
0.000 |
z |
0.000 |
0.000 |
-35.232 |
|
Traceless |
| x | y | z |
x |
-1.916 |
0.000 |
0.000 |
y |
0.000 |
-1.916 |
0.000 |
z |
0.000 |
0.000 |
3.833 |
|
Polar |
3z2-r2 | 7.665 |
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 |
3.932 |
0.000 |
0.000 |
y |
0.000 |
3.932 |
0.000 |
z |
0.000 |
0.000 |
2.520 |
<r2> (average value of r
2) Å
2
<r2> |
142.422 |
(<r2>)1/2 |
11.934 |