Vibrational Frequencies calculated at ROHF/cc-pVTZ
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 |
1012 |
912 |
190.11 |
|
|
|
2 |
A1 |
739 |
666 |
23.09 |
|
|
|
3 |
A1 |
638 |
575 |
44.27 |
|
|
|
4 |
B1 |
526 |
474 |
0.00 |
|
|
|
5 |
B2 |
678 |
611 |
0.00 |
|
|
|
6 |
B2 |
280 |
252 |
0.00 |
|
|
|
7 |
E |
959 |
864 |
569.16 |
|
|
|
7 |
E |
959 |
864 |
569.16 |
|
|
|
8 |
E |
598 |
539 |
9.41 |
|
|
|
8 |
E |
598 |
539 |
9.41 |
|
|
|
9 |
E |
408 |
367 |
0.21 |
|
|
|
9 |
E |
408 |
367 |
0.21 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3900.8 cm
-1
Scaled (by 0.901) Zero Point Vibrational Energy (zpe) 3514.6 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 ROHF/cc-pVTZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
S |
1.299 |
|
|
|
2 |
F |
-0.203 |
|
|
|
3 |
F |
-0.274 |
|
|
|
4 |
F |
-0.274 |
|
|
|
5 |
F |
-0.274 |
|
|
|
6 |
F |
-0.274 |
|
|
|
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 |
0.489 |
0.489 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-38.970 |
0.000 |
0.000 |
y |
0.000 |
-38.970 |
0.000 |
z |
0.000 |
0.000 |
-35.407 |
|
Traceless |
| x | y | z |
x |
-1.782 |
0.000 |
0.000 |
y |
0.000 |
-1.782 |
0.000 |
z |
0.000 |
0.000 |
3.564 |
|
Polar |
3z2-r2 | 7.127 |
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 |
0.000 |
0.000 |
0.000 |
y |
0.000 |
0.000 |
0.000 |
z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
<r2> |
129.968 |
(<r2>)1/2 |
11.400 |