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' |
3196 |
3031 |
7.85 |
|
|
|
| 2 |
A' |
1365 |
1295 |
26.41 |
|
|
|
| 3 |
A' |
1162 |
1103 |
193.36 |
|
|
|
| 4 |
A' |
755 |
716 |
48.59 |
|
|
|
| 5 |
A' |
465 |
441 |
2.33 |
|
|
|
| 6 |
A' |
285 |
270 |
0.27 |
|
|
|
| 7 |
A" |
1311 |
1244 |
71.10 |
|
|
|
| 8 |
A" |
816 |
774 |
264.02 |
|
|
|
| 9 |
A" |
372 |
353 |
0.04 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4863.8 cm
-1
Scaled (by 0.9485) Zero Point Vibrational Energy (zpe) 4613.3 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 |
-0.032 |
|
|
|
| 2 |
H |
0.250 |
|
|
|
| 3 |
F |
-0.229 |
|
|
|
| 4 |
Cl |
0.006 |
|
|
|
| 5 |
Cl |
0.006 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.157 |
0.833 |
0.000 |
1.426 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-35.454 |
-1.758 |
0.000 |
| y |
-1.758 |
-35.204 |
0.000 |
| z |
0.000 |
0.000 |
-36.502 |
|
| Traceless |
| | x | y | z |
| x |
0.399 |
-1.758 |
0.000 |
| y |
-1.758 |
0.774 |
0.000 |
| z |
0.000 |
0.000 |
-1.173 |
|
| Polar |
| 3z2-r2 | -2.345 |
| x2-y2 | -0.250 |
| xy | -1.758 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.154 |
0.125 |
0.000 |
| y |
0.125 |
4.077 |
0.000 |
| z |
0.000 |
0.000 |
6.161 |
<r2> (average value of r
2) Å
2
| <r2> |
131.617 |
| (<r2>)1/2 |
11.472 |