Vibrational Frequencies calculated at PBEPBE/6-31G**
| 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' |
3006 |
2965 |
29.02 |
|
|
|
| 2 |
A' |
1470 |
1450 |
0.67 |
|
|
|
| 3 |
A' |
1337 |
1319 |
45.08 |
|
|
|
| 4 |
A' |
1096 |
1081 |
157.15 |
|
|
|
| 5 |
A' |
711 |
701 |
101.85 |
|
|
|
| 6 |
A' |
367 |
362 |
1.41 |
|
|
|
| 7 |
A" |
3081 |
3038 |
19.25 |
|
|
|
| 8 |
A" |
1215 |
1199 |
1.77 |
|
|
|
| 9 |
A" |
986 |
972 |
0.27 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6634.9 cm
-1
Scaled (by 0.9863) Zero Point Vibrational Energy (zpe) 6544.0 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 PBEPBE/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.036 |
|
|
|
| 2 |
F |
-0.229 |
|
|
|
| 3 |
Cl |
-0.062 |
|
|
|
| 4 |
H |
0.164 |
|
|
|
| 5 |
H |
0.164 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.681 |
1.724 |
0.000 |
1.853 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.484 |
-1.301 |
0.000 |
| y |
-1.301 |
-22.418 |
0.000 |
| z |
0.000 |
0.000 |
-23.184 |
|
| Traceless |
| | x | y | z |
| x |
-2.683 |
-1.301 |
0.000 |
| y |
-1.301 |
1.917 |
0.000 |
| z |
0.000 |
0.000 |
0.767 |
|
| Polar |
| 3z2-r2 | 1.533 |
| x2-y2 | -3.067 |
| xy | -1.301 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.035 |
0.754 |
0.000 |
| y |
0.754 |
4.153 |
0.000 |
| z |
0.000 |
0.000 |
2.571 |
<r2> (average value of r
2) Å
2
| <r2> |
66.739 |
| (<r2>)1/2 |
8.169 |