Vibrational Frequencies calculated at LSDA/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 |
874 |
865 |
137.48 |
|
|
|
2 |
A1 |
630 |
623 |
4.67 |
|
|
|
3 |
A1 |
461 |
456 |
24.22 |
|
|
|
4 |
B1 |
396 |
391 |
0.00 |
|
|
|
5 |
B2 |
599 |
592 |
0.00 |
|
|
|
6 |
B2 |
204 |
202 |
0.00 |
|
|
|
7 |
E |
851 |
842 |
385.25 |
|
|
|
7 |
E |
851 |
842 |
385.25 |
|
|
|
8 |
E |
450 |
445 |
3.59 |
|
|
|
8 |
E |
450 |
445 |
3.59 |
|
|
|
9 |
E |
310 |
307 |
0.11 |
|
|
|
9 |
E |
310 |
307 |
0.11 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3193.0 cm
-1
Scaled (by 0.989) Zero Point Vibrational Energy (zpe) 3157.9 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/cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
S |
1.082 |
|
|
|
2 |
F |
-0.185 |
|
|
|
3 |
F |
-0.224 |
|
|
|
4 |
F |
-0.224 |
|
|
|
5 |
F |
-0.224 |
|
|
|
6 |
F |
-0.224 |
|
|
|
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 |
0.419 |
0.419 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-38.649 |
0.000 |
0.000 |
y |
0.000 |
-38.649 |
0.000 |
z |
0.000 |
0.000 |
-35.345 |
|
Traceless |
| x | y | z |
x |
-1.652 |
0.000 |
0.000 |
y |
0.000 |
-1.652 |
0.000 |
z |
0.000 |
0.000 |
3.303 |
|
Polar |
3z2-r2 | 6.607 |
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 |
4.033 |
0.000 |
0.000 |
y |
0.000 |
4.033 |
0.000 |
z |
0.000 |
0.000 |
2.600 |
<r2> (average value of r
2) Å
2
<r2> |
141.875 |
(<r2>)1/2 |
11.911 |