Vibrational Frequencies calculated at B3LYP/6-31G(2df,p)
| 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' |
3144 |
3034 |
4.64 |
|
|
|
| 2 |
A' |
1340 |
1293 |
18.41 |
|
|
|
| 3 |
A' |
1143 |
1103 |
173.01 |
|
|
|
| 4 |
A' |
721 |
696 |
42.89 |
|
|
|
| 5 |
A' |
451 |
435 |
1.88 |
|
|
|
| 6 |
A' |
268 |
259 |
0.13 |
|
|
|
| 7 |
A" |
1244 |
1200 |
59.46 |
|
|
|
| 8 |
A" |
761 |
735 |
256.59 |
|
|
|
| 9 |
A" |
362 |
350 |
0.18 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4717.5 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 4552.4 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 B3LYP/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.109 |
|
|
|
| 2 |
H |
0.179 |
|
|
|
| 3 |
F |
-0.067 |
|
|
|
| 4 |
Cl |
-0.111 |
|
|
|
| 5 |
Cl |
-0.111 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.985 |
0.827 |
0.000 |
1.287 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-35.466 |
-1.692 |
0.000 |
| y |
-1.692 |
-35.043 |
0.000 |
| z |
0.000 |
0.000 |
-36.253 |
|
| Traceless |
| | x | y | z |
| x |
0.182 |
-1.692 |
0.000 |
| y |
-1.692 |
0.816 |
0.000 |
| z |
0.000 |
0.000 |
-0.998 |
|
| Polar |
| 3z2-r2 | -1.997 |
| x2-y2 | -0.423 |
| xy | -1.692 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.049 |
0.145 |
0.000 |
| y |
0.145 |
4.854 |
0.000 |
| z |
0.000 |
0.000 |
7.006 |
<r2> (average value of r
2) Å
2
| <r2> |
132.288 |
| (<r2>)1/2 |
11.502 |