Vibrational Frequencies calculated at PBEPBE/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' |
3012 |
2980 |
32.35 |
|
|
|
| 2 |
A' |
1463 |
1448 |
0.36 |
|
|
|
| 3 |
A' |
1349 |
1335 |
45.01 |
|
|
|
| 4 |
A' |
1061 |
1050 |
175.26 |
|
|
|
| 5 |
A' |
706 |
699 |
111.93 |
|
|
|
| 6 |
A' |
370 |
366 |
1.16 |
|
|
|
| 7 |
A" |
3089 |
3057 |
19.68 |
|
|
|
| 8 |
A" |
1228 |
1216 |
3.33 |
|
|
|
| 9 |
A" |
989 |
978 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6633.4 cm
-1
Scaled (by 0.9896) Zero Point Vibrational Energy (zpe) 6564.4 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 PBEPBE/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.227 |
|
|
|
| 2 |
F |
-0.186 |
|
|
|
| 3 |
Cl |
-0.086 |
|
|
|
| 4 |
H |
0.249 |
|
|
|
| 5 |
H |
0.249 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.853 |
1.747 |
0.000 |
1.944 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.312 |
-1.375 |
0.000 |
| y |
-1.375 |
-22.876 |
0.000 |
| z |
0.000 |
0.000 |
-23.623 |
|
| Traceless |
| | x | y | z |
| x |
-3.062 |
-1.375 |
0.000 |
| y |
-1.375 |
2.092 |
0.000 |
| z |
0.000 |
0.000 |
0.970 |
|
| Polar |
| 3z2-r2 | 1.941 |
| x2-y2 | -3.436 |
| xy | -1.375 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.012 |
0.887 |
0.000 |
| y |
0.887 |
4.341 |
0.000 |
| z |
0.000 |
0.000 |
2.435 |
<r2> (average value of r
2) Å
2
| <r2> |
67.024 |
| (<r2>)1/2 |
8.187 |