Vibrational Frequencies calculated at B3LYP/cc-pVDZ
| 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' |
3075 |
2983 |
26.08 |
|
|
|
| 2 |
A' |
1477 |
1433 |
1.09 |
|
|
|
| 3 |
A' |
1348 |
1308 |
43.59 |
|
|
|
| 4 |
A' |
1100 |
1067 |
175.24 |
|
|
|
| 5 |
A' |
726 |
704 |
99.79 |
|
|
|
| 6 |
A' |
376 |
365 |
1.20 |
|
|
|
| 7 |
A" |
3157 |
3062 |
15.09 |
|
|
|
| 8 |
A" |
1236 |
1199 |
3.41 |
|
|
|
| 9 |
A" |
987 |
957 |
0.55 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6740.5 cm
-1
Scaled (by 0.97) Zero Point Vibrational Energy (zpe) 6538.3 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 B3LYP/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.190 |
|
|
|
| 2 |
F |
-0.193 |
|
|
|
| 3 |
Cl |
-0.137 |
|
|
|
| 4 |
H |
0.070 |
|
|
|
| 5 |
H |
0.070 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.859 |
1.641 |
0.000 |
1.852 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.746 |
-1.403 |
0.000 |
| y |
-1.403 |
-22.294 |
0.000 |
| z |
0.000 |
0.000 |
-23.062 |
|
| Traceless |
| | x | y | z |
| x |
-3.067 |
-1.403 |
0.000 |
| y |
-1.403 |
2.110 |
0.000 |
| z |
0.000 |
0.000 |
0.958 |
|
| Polar |
| 3z2-r2 | 1.915 |
| x2-y2 | -3.451 |
| xy | -1.403 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.888 |
0.757 |
0.000 |
| y |
0.757 |
4.073 |
0.000 |
| z |
0.000 |
0.000 |
2.419 |
<r2> (average value of r
2) Å
2
| <r2> |
0.000 |
| (<r2>)1/2 |
0.000 |