Vibrational Frequencies calculated at wB97X-D/SDD
| 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' |
3173 |
3173 |
25.21 |
|
|
|
| 2 |
A' |
1491 |
1491 |
0.26 |
|
|
|
| 3 |
A' |
1366 |
1366 |
53.84 |
|
|
|
| 4 |
A' |
1018 |
1018 |
177.87 |
|
|
|
| 5 |
A' |
624 |
624 |
71.58 |
|
|
|
| 6 |
A' |
298 |
298 |
1.18 |
|
|
|
| 7 |
A" |
3279 |
3279 |
10.75 |
|
|
|
| 8 |
A" |
1229 |
1229 |
3.54 |
|
|
|
| 9 |
A" |
944 |
944 |
0.61 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6711.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 6711.4 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/SDD
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.317 |
|
|
|
| 2 |
F |
-0.241 |
|
|
|
| 3 |
Br |
0.025 |
|
|
|
| 4 |
H |
0.267 |
|
|
|
| 5 |
H |
0.267 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.390 |
-0.463 |
0.000 |
2.434 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.927 |
-4.253 |
0.000 |
| y |
-4.253 |
-27.657 |
0.000 |
| z |
0.000 |
0.000 |
-25.748 |
|
| Traceless |
| | x | y | z |
| x |
0.775 |
-4.253 |
0.000 |
| y |
-4.253 |
-1.820 |
0.000 |
| z |
0.000 |
0.000 |
1.045 |
|
| Polar |
| 3z2-r2 | 2.089 |
| x2-y2 | 1.730 |
| xy | -4.253 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.081 |
-0.687 |
0.000 |
| y |
-0.687 |
5.583 |
0.000 |
| z |
0.000 |
0.000 |
1.797 |
<r2> (average value of r
2) Å
2
| <r2> |
75.660 |
| (<r2>)1/2 |
8.698 |