Vibrational Frequencies calculated at B3PW91/6-31G
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A' |
3227 |
3091 |
1.98 |
|
|
|
| 2 |
A' |
1301 |
1246 |
14.48 |
|
|
|
| 3 |
A' |
1062 |
1018 |
169.50 |
|
|
|
| 4 |
A' |
592 |
567 |
31.50 |
|
|
|
| 5 |
A' |
334 |
320 |
1.52 |
|
|
|
| 6 |
A' |
167 |
160 |
0.07 |
|
|
|
| 7 |
A" |
1193 |
1142 |
77.28 |
|
|
|
| 8 |
A" |
652 |
624 |
221.96 |
|
|
|
| 9 |
A" |
279 |
267 |
0.06 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4403.4 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 4217.1 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 B3PW91/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.304 |
|
|
|
| 2 |
H |
0.287 |
|
|
|
| 3 |
F |
-0.255 |
|
|
|
| 4 |
Br |
0.136 |
|
|
|
| 5 |
Br |
0.136 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.571 |
0.433 |
0.000 |
1.630 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-47.885 |
-2.654 |
0.000 |
| y |
-2.654 |
-47.053 |
0.000 |
| z |
0.000 |
0.000 |
-47.476 |
|
| Traceless |
| | x | y | z |
| x |
-0.620 |
-2.654 |
0.000 |
| y |
-2.654 |
0.628 |
0.000 |
| z |
0.000 |
0.000 |
-0.007 |
|
| Polar |
| 3z2-r2 | -0.015 |
| x2-y2 | -0.832 |
| xy | -2.654 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.717 |
0.298 |
0.000 |
| y |
0.298 |
4.405 |
0.000 |
| z |
0.000 |
0.000 |
8.336 |
<r2> (average value of r
2) Å
2
| <r2> |
262.662 |
| (<r2>)1/2 |
16.207 |