Vibrational Frequencies calculated at wB97X-D/CEP-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' |
3154 |
3154 |
38.03 |
|
|
|
| 2 |
A' |
1486 |
1486 |
0.14 |
|
|
|
| 3 |
A' |
1358 |
1358 |
59.59 |
|
|
|
| 4 |
A' |
1024 |
1024 |
176.63 |
|
|
|
| 5 |
A' |
618 |
618 |
76.70 |
|
|
|
| 6 |
A' |
295 |
295 |
1.21 |
|
|
|
| 7 |
A" |
3266 |
3266 |
19.15 |
|
|
|
| 8 |
A" |
1221 |
1221 |
2.90 |
|
|
|
| 9 |
A" |
936 |
936 |
0.53 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6678.7 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 6678.7 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 wB97X-D/CEP-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.296 |
|
|
|
| 2 |
F |
-0.210 |
|
|
|
| 3 |
Br |
0.046 |
|
|
|
| 4 |
H |
0.230 |
|
|
|
| 5 |
H |
0.230 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.454 |
-0.427 |
0.000 |
2.491 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.896 |
-4.349 |
0.000 |
| y |
-4.349 |
-27.816 |
0.000 |
| z |
0.000 |
0.000 |
-25.661 |
|
| Traceless |
| | x | y | z |
| x |
0.842 |
-4.349 |
0.000 |
| y |
-4.349 |
-2.037 |
0.000 |
| z |
0.000 |
0.000 |
1.195 |
|
| Polar |
| 3z2-r2 | 2.391 |
| x2-y2 | 1.920 |
| xy | -4.349 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.275 |
-0.654 |
0.000 |
| y |
-0.654 |
5.703 |
0.000 |
| z |
0.000 |
0.000 |
1.847 |
<r2> (average value of r
2) Å
2
| <r2> |
64.307 |
| (<r2>)1/2 |
8.019 |