Vibrational Frequencies calculated at B3LYP/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' |
3088 |
2986 |
26.85 |
|
|
|
| 2 |
A' |
1500 |
1450 |
0.58 |
|
|
|
| 3 |
A' |
1378 |
1333 |
47.16 |
|
|
|
| 4 |
A' |
1085 |
1049 |
180.01 |
|
|
|
| 5 |
A' |
722 |
698 |
111.92 |
|
|
|
| 6 |
A' |
378 |
365 |
1.26 |
|
|
|
| 7 |
A" |
3167 |
3062 |
13.57 |
|
|
|
| 8 |
A" |
1257 |
1216 |
3.97 |
|
|
|
| 9 |
A" |
1006 |
972 |
0.08 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6790.6 cm
-1
Scaled (by 0.9668) Zero Point Vibrational Energy (zpe) 6565.1 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/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.026 |
|
|
|
| 2 |
F |
-0.222 |
|
|
|
| 3 |
Cl |
-0.113 |
|
|
|
| 4 |
H |
0.155 |
|
|
|
| 5 |
H |
0.155 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.962 |
1.797 |
0.000 |
2.039 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.529 |
-1.481 |
0.000 |
| y |
-1.481 |
-22.825 |
0.000 |
| z |
0.000 |
0.000 |
-23.579 |
|
| Traceless |
| | x | y | z |
| x |
-3.327 |
-1.481 |
0.000 |
| y |
-1.481 |
2.229 |
0.000 |
| z |
0.000 |
0.000 |
1.098 |
|
| Polar |
| 3z2-r2 | 2.197 |
| x2-y2 | -3.704 |
| xy | -1.481 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.940 |
0.862 |
0.000 |
| y |
0.862 |
4.277 |
0.000 |
| z |
0.000 |
0.000 |
2.392 |
<r2> (average value of r
2) Å
2
| <r2> |
66.689 |
| (<r2>)1/2 |
8.166 |