Vibrational Frequencies calculated at B3LYP/Def2TZVPP
| 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' |
3149 |
3031 |
2.78 |
|
|
|
| 2 |
A' |
1334 |
1284 |
12.30 |
|
|
|
| 3 |
A' |
1081 |
1040 |
193.57 |
|
|
|
| 4 |
A' |
722 |
695 |
44.62 |
|
|
|
| 5 |
A' |
451 |
434 |
1.15 |
|
|
|
| 6 |
A' |
271 |
261 |
0.02 |
|
|
|
| 7 |
A" |
1251 |
1204 |
50.28 |
|
|
|
| 8 |
A" |
764 |
735 |
251.63 |
|
|
|
| 9 |
A" |
362 |
348 |
0.05 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4692.0 cm
-1
Scaled (by 0.9626) Zero Point Vibrational Energy (zpe) 4516.5 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/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.162 |
|
|
|
| 2 |
H |
0.154 |
|
|
|
| 3 |
F |
-0.161 |
|
|
|
| 4 |
Cl |
-0.077 |
|
|
|
| 5 |
Cl |
-0.077 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.154 |
0.534 |
0.000 |
1.271 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-36.049 |
-1.950 |
0.000 |
| y |
-1.950 |
-35.708 |
0.000 |
| z |
0.000 |
0.000 |
-36.221 |
|
| Traceless |
| | x | y | z |
| x |
-0.085 |
-1.950 |
0.000 |
| y |
-1.950 |
0.428 |
0.000 |
| z |
0.000 |
0.000 |
-0.343 |
|
| Polar |
| 3z2-r2 | -0.685 |
| x2-y2 | -0.342 |
| xy | -1.950 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.316 |
0.186 |
0.000 |
| y |
0.186 |
5.136 |
0.000 |
| z |
0.000 |
0.000 |
7.248 |
<r2> (average value of r
2) Å
2
| <r2> |
132.185 |
| (<r2>)1/2 |
11.497 |