Vibrational Frequencies calculated at B3LYP/aug-cc-pVTZ
| 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' |
3152 |
3050 |
0.87 |
|
|
|
| 2 |
A' |
1329 |
1285 |
10.53 |
|
|
|
| 3 |
A' |
1076 |
1041 |
187.37 |
|
|
|
| 4 |
A' |
719 |
695 |
43.03 |
|
|
|
| 5 |
A' |
449 |
435 |
1.10 |
|
|
|
| 6 |
A' |
270 |
261 |
0.01 |
|
|
|
| 7 |
A" |
1247 |
1207 |
48.43 |
|
|
|
| 8 |
A" |
759 |
734 |
249.20 |
|
|
|
| 9 |
A" |
361 |
349 |
0.05 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4680.8 cm
-1
Scaled (by 0.9675) Zero Point Vibrational Energy (zpe) 4528.7 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/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.330 |
|
|
|
| 2 |
H |
0.254 |
|
|
|
| 3 |
F |
-0.339 |
|
|
|
| 4 |
Cl |
-0.122 |
|
|
|
| 5 |
Cl |
-0.122 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.150 |
0.560 |
0.000 |
1.279 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-36.385 |
-2.018 |
0.000 |
| y |
-2.018 |
-35.975 |
0.000 |
| z |
0.000 |
0.000 |
-36.589 |
|
| Traceless |
| | x | y | z |
| x |
-0.102 |
-2.018 |
0.000 |
| y |
-2.018 |
0.512 |
0.000 |
| z |
0.000 |
0.000 |
-0.410 |
|
| Polar |
| 3z2-r2 | -0.819 |
| x2-y2 | -0.410 |
| xy | -2.018 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.516 |
0.211 |
0.000 |
| y |
0.211 |
6.173 |
0.000 |
| z |
0.000 |
0.000 |
8.275 |
<r2> (average value of r
2) Å
2
| <r2> |
132.745 |
| (<r2>)1/2 |
11.522 |