Vibrational Frequencies calculated at wB97X-D/TZVP
| 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' |
3122 |
2981 |
16.81 |
|
|
|
| 2 |
A' |
1502 |
1434 |
1.31 |
|
|
|
| 3 |
A' |
1358 |
1297 |
60.20 |
|
|
|
| 4 |
A' |
1101 |
1052 |
214.66 |
|
|
|
| 5 |
A' |
657 |
628 |
72.27 |
|
|
|
| 6 |
A' |
319 |
304 |
0.52 |
|
|
|
| 7 |
A" |
3207 |
3063 |
5.10 |
|
|
|
| 8 |
A" |
1268 |
1211 |
2.89 |
|
|
|
| 9 |
A" |
942 |
900 |
0.02 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6738.0 cm
-1
Scaled (by 0.955) Zero Point Vibrational Energy (zpe) 6434.8 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/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.029 |
|
|
|
| 2 |
F |
-0.193 |
|
|
|
| 3 |
Br |
-0.119 |
|
|
|
| 4 |
H |
0.142 |
|
|
|
| 5 |
H |
0.142 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.814 |
-0.620 |
0.000 |
1.917 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-29.326 |
-3.424 |
0.000 |
| y |
-3.424 |
-30.104 |
0.000 |
| z |
0.000 |
0.000 |
-29.190 |
|
| Traceless |
| | x | y | z |
| x |
0.322 |
-3.424 |
0.000 |
| y |
-3.424 |
-0.846 |
0.000 |
| z |
0.000 |
0.000 |
0.525 |
|
| Polar |
| 3z2-r2 | 1.050 |
| x2-y2 | 0.779 |
| xy | -3.424 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.562 |
-0.487 |
0.000 |
| y |
-0.487 |
5.920 |
0.000 |
| z |
0.000 |
0.000 |
3.324 |
<r2> (average value of r
2) Å
2
| <r2> |
91.078 |
| (<r2>)1/2 |
9.543 |