Vibrational Frequencies calculated at B3LYP/3-21G*
| 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' |
3175 |
3054 |
6.68 |
|
|
|
| 2 |
A' |
1347 |
1296 |
14.58 |
|
|
|
| 3 |
A' |
1099 |
1057 |
131.03 |
|
|
|
| 4 |
A' |
694 |
667 |
49.39 |
|
|
|
| 5 |
A' |
419 |
403 |
3.70 |
|
|
|
| 6 |
A' |
270 |
260 |
0.35 |
|
|
|
| 7 |
A" |
1291 |
1242 |
49.67 |
|
|
|
| 8 |
A" |
691 |
665 |
279.35 |
|
|
|
| 9 |
A" |
334 |
321 |
0.39 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4659.7 cm
-1
Scaled (by 0.962) Zero Point Vibrational Energy (zpe) 4482.6 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/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.078 |
|
|
|
| 2 |
H |
0.285 |
|
|
|
| 3 |
F |
-0.244 |
|
|
|
| 4 |
Cl |
0.018 |
|
|
|
| 5 |
Cl |
0.018 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.304 |
0.770 |
0.000 |
1.515 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-35.912 |
-1.979 |
0.000 |
| y |
-1.979 |
-35.715 |
0.000 |
| z |
0.000 |
0.000 |
-36.889 |
|
| Traceless |
| | x | y | z |
| x |
0.389 |
-1.979 |
0.000 |
| y |
-1.979 |
0.686 |
0.000 |
| z |
0.000 |
0.000 |
-1.075 |
|
| Polar |
| 3z2-r2 | -2.150 |
| x2-y2 | -0.198 |
| xy | -1.979 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.915 |
0.204 |
0.000 |
| y |
0.204 |
3.895 |
0.000 |
| z |
0.000 |
0.000 |
6.143 |
<r2> (average value of r
2) Å
2
| <r2> |
0.000 |
| (<r2>)1/2 |
0.000 |