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' |
3067 |
3035 |
28.94 |
|
|
|
| 2 |
A' |
1290 |
1276 |
77.29 |
|
|
|
| 3 |
A' |
1077 |
1066 |
234.76 |
|
|
|
| 4 |
A' |
754 |
747 |
183.55 |
|
|
|
| 5 |
A' |
577 |
571 |
8.40 |
|
|
|
| 6 |
A' |
388 |
384 |
1.37 |
|
|
|
| 7 |
A" |
1341 |
1327 |
24.76 |
|
|
|
| 8 |
A" |
1099 |
1087 |
246.61 |
|
|
|
| 9 |
A" |
351 |
347 |
0.73 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4971.6 cm
-1
Scaled (by 0.9896) Zero Point Vibrational Energy (zpe) 4919.9 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 |
0.140 |
|
|
|
| 2 |
H |
0.240 |
|
|
|
| 3 |
Cl |
-0.073 |
|
|
|
| 4 |
F |
-0.154 |
|
|
|
| 5 |
F |
-0.154 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.343 |
0.672 |
0.000 |
1.502 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.701 |
-1.022 |
0.000 |
| y |
-1.022 |
-29.211 |
0.000 |
| z |
0.000 |
0.000 |
-30.108 |
|
| Traceless |
| | x | y | z |
| x |
2.958 |
-1.022 |
0.000 |
| y |
-1.022 |
-0.806 |
0.000 |
| z |
0.000 |
0.000 |
-2.152 |
|
| Polar |
| 3z2-r2 | -4.304 |
| x2-y2 | 2.509 |
| xy | -1.022 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.922 |
1.135 |
0.000 |
| y |
1.135 |
3.420 |
0.000 |
| z |
0.000 |
0.000 |
2.673 |
<r2> (average value of r
2) Å
2
| <r2> |
92.639 |
| (<r2>)1/2 |
9.625 |