Vibrational Frequencies calculated at wB97X-D/6-311G**
| 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' |
3178 |
3040 |
7.29 |
|
|
|
| 2 |
A' |
1350 |
1291 |
23.09 |
|
|
|
| 3 |
A' |
1128 |
1079 |
220.17 |
|
|
|
| 4 |
A' |
746 |
714 |
48.62 |
|
|
|
| 5 |
A' |
465 |
445 |
1.82 |
|
|
|
| 6 |
A' |
286 |
274 |
0.06 |
|
|
|
| 7 |
A" |
1286 |
1231 |
69.31 |
|
|
|
| 8 |
A" |
809 |
774 |
283.34 |
|
|
|
| 9 |
A" |
376 |
360 |
0.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4812.3 cm
-1
Scaled (by 0.9565) Zero Point Vibrational Energy (zpe) 4603.0 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/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.007 |
|
|
|
| 2 |
H |
0.213 |
|
|
|
| 3 |
F |
-0.174 |
|
|
|
| 4 |
Cl |
-0.023 |
|
|
|
| 5 |
Cl |
-0.023 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.273 |
0.709 |
0.000 |
1.457 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-36.248 |
-1.888 |
0.000 |
| y |
-1.888 |
-35.937 |
0.000 |
| z |
0.000 |
0.000 |
-37.056 |
|
| Traceless |
| | x | y | z |
| x |
0.249 |
-1.888 |
0.000 |
| y |
-1.888 |
0.715 |
0.000 |
| z |
0.000 |
0.000 |
-0.964 |
|
| Polar |
| 3z2-r2 | -1.927 |
| x2-y2 | -0.311 |
| xy | -1.888 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.979 |
0.143 |
0.000 |
| y |
0.143 |
4.100 |
0.000 |
| z |
0.000 |
0.000 |
6.456 |
<r2> (average value of r
2) Å
2
| <r2> |
131.947 |
| (<r2>)1/2 |
11.487 |