Vibrational Frequencies calculated at PBEPBE/6-31G
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 |
511 |
504 |
20.65 |
|
|
|
2 |
A1 |
458 |
452 |
5.62 |
|
|
|
3 |
A1 |
215 |
212 |
27.76 |
|
|
|
4 |
B1 |
204 |
201 |
0.00 |
|
|
|
5 |
B2 |
439 |
433 |
0.00 |
|
|
|
6 |
B2 |
145 |
143 |
0.00 |
|
|
|
7 |
E |
573 |
565 |
121.71 |
|
|
|
7 |
E |
573 |
565 |
121.71 |
|
|
|
8 |
E |
260 |
256 |
4.12 |
|
|
|
8 |
E |
260 |
256 |
4.12 |
|
|
|
9 |
E |
140 |
138 |
3.50 |
|
|
|
9 |
E |
140 |
138 |
3.50 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1958.7 cm
-1
Scaled (by 0.9862) Zero Point Vibrational Energy (zpe) 1931.7 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 PBEPBE/6-31G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Br |
1.604 |
|
|
|
2 |
F |
-0.276 |
|
|
|
3 |
F |
-0.332 |
|
|
|
4 |
F |
-0.332 |
|
|
|
5 |
F |
-0.332 |
|
|
|
6 |
F |
-0.332 |
|
|
|
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 |
2.416 |
2.416 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-48.070 |
0.000 |
0.000 |
y |
0.000 |
-48.070 |
0.000 |
z |
0.000 |
0.000 |
-40.633 |
|
Traceless |
| x | y | z |
x |
-3.718 |
0.000 |
0.000 |
y |
0.000 |
-3.718 |
0.000 |
z |
0.000 |
0.000 |
7.436 |
|
Polar |
3z2-r2 | 14.873 |
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 |
6.523 |
0.000 |
0.000 |
y |
0.000 |
6.523 |
0.000 |
z |
0.000 |
0.000 |
3.390 |
<r2> (average value of r
2) Å
2
<r2> |
0.000 |
(<r2>)1/2 |
0.000 |