Vibrational Frequencies calculated at B3LYP/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 |
861 |
835 |
142.77 |
|
|
|
2 |
A1 |
608 |
590 |
4.77 |
|
|
|
3 |
A1 |
474 |
460 |
30.36 |
|
|
|
4 |
B1 |
402 |
390 |
0.00 |
|
|
|
5 |
B2 |
582 |
564 |
0.00 |
|
|
|
6 |
B2 |
207 |
200 |
0.00 |
|
|
|
7 |
E |
816 |
792 |
402.84 |
|
|
|
7 |
E |
816 |
792 |
402.84 |
|
|
|
8 |
E |
455 |
441 |
2.22 |
|
|
|
8 |
E |
455 |
441 |
2.22 |
|
|
|
9 |
E |
314 |
304 |
0.04 |
|
|
|
9 |
E |
314 |
304 |
0.04 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3150.8 cm
-1
Scaled (by 0.97) Zero Point Vibrational Energy (zpe) 3056.3 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 B3LYP/cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
S |
1.317 |
|
|
|
2 |
F |
-0.228 |
|
|
|
3 |
F |
-0.272 |
|
|
|
4 |
F |
-0.272 |
|
|
|
5 |
F |
-0.272 |
|
|
|
6 |
F |
-0.272 |
|
|
|
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 |
0.512 |
0.512 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-39.207 |
0.000 |
0.000 |
y |
0.000 |
-39.207 |
0.000 |
z |
0.000 |
0.000 |
-35.262 |
|
Traceless |
| x | y | z |
x |
-1.973 |
0.000 |
0.000 |
y |
0.000 |
-1.973 |
0.000 |
z |
0.000 |
0.000 |
3.945 |
|
Polar |
3z2-r2 | 7.890 |
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 |
4.016 |
0.000 |
0.000 |
y |
0.000 |
4.016 |
0.000 |
z |
0.000 |
0.000 |
2.539 |
<r2> (average value of r
2) Å
2
<r2> |
143.839 |
(<r2>)1/2 |
11.993 |