Vibrational Frequencies calculated at wB97X-D/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' |
3172 |
3172 |
14.88 |
|
|
|
| 2 |
A' |
1523 |
1523 |
0.41 |
|
|
|
| 3 |
A' |
1370 |
1370 |
46.68 |
|
|
|
| 4 |
A' |
1058 |
1058 |
147.81 |
|
|
|
| 5 |
A' |
619 |
619 |
70.93 |
|
|
|
| 6 |
A' |
298 |
298 |
1.11 |
|
|
|
| 7 |
A" |
3273 |
3273 |
7.81 |
|
|
|
| 8 |
A" |
1242 |
1242 |
2.06 |
|
|
|
| 9 |
A" |
943 |
943 |
0.02 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6749.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 6749.5 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 wB97X-D/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.197 |
|
|
|
| 2 |
F |
-0.309 |
|
|
|
| 3 |
Br |
0.042 |
|
|
|
| 4 |
H |
0.232 |
|
|
|
| 5 |
H |
0.232 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.220 |
-0.580 |
0.000 |
2.294 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-29.011 |
-3.743 |
0.000 |
| y |
-3.743 |
-30.836 |
0.000 |
| z |
0.000 |
0.000 |
-28.928 |
|
| Traceless |
| | x | y | z |
| x |
0.871 |
-3.743 |
0.000 |
| y |
-3.743 |
-1.867 |
0.000 |
| z |
0.000 |
0.000 |
0.996 |
|
| Polar |
| 3z2-r2 | 1.992 |
| x2-y2 | 1.825 |
| xy | -3.743 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.367 |
-0.594 |
0.000 |
| y |
-0.594 |
5.297 |
0.000 |
| z |
0.000 |
0.000 |
2.079 |
<r2> (average value of r
2) Å
2
| <r2> |
93.828 |
| (<r2>)1/2 |
9.686 |