Vibrational Frequencies calculated at HSEh1PBE/3-21G
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 |
624 |
601 |
39.86 |
|
|
|
2 |
A1 |
487 |
469 |
7.23 |
|
|
|
3 |
A1 |
347 |
334 |
32.26 |
|
|
|
4 |
B1 |
251 |
242 |
0.00 |
|
|
|
5 |
B2 |
478 |
461 |
0.00 |
|
|
|
6 |
B2 |
180 |
173 |
0.00 |
|
|
|
7 |
E |
766 |
737 |
216.94 |
|
|
|
7 |
E |
766 |
737 |
216.94 |
|
|
|
8 |
E |
327 |
315 |
2.54 |
|
|
|
8 |
E |
327 |
315 |
2.54 |
|
|
|
9 |
E |
195 |
188 |
1.01 |
|
|
|
9 |
E |
195 |
188 |
1.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2470.9 cm
-1
Scaled (by 0.9633) Zero Point Vibrational Energy (zpe) 2380.3 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 HSEh1PBE/3-21G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
1.376 |
|
|
|
2 |
F |
-0.219 |
|
|
|
3 |
F |
-0.289 |
|
|
|
4 |
F |
-0.289 |
|
|
|
5 |
F |
-0.289 |
|
|
|
6 |
F |
-0.289 |
|
|
|
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 |
1.545 |
1.545 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-39.950 |
0.000 |
0.000 |
y |
0.000 |
-39.950 |
0.000 |
z |
0.000 |
0.000 |
-33.968 |
|
Traceless |
| x | y | z |
x |
-2.991 |
0.000 |
0.000 |
y |
0.000 |
-2.991 |
0.000 |
z |
0.000 |
0.000 |
5.981 |
|
Polar |
3z2-r2 | 11.963 |
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 |
5.246 |
0.000 |
0.000 |
y |
0.000 |
5.246 |
0.000 |
z |
0.000 |
0.000 |
2.544 |
<r2> (average value of r
2) Å
2
<r2> |
159.491 |
(<r2>)1/2 |
12.629 |