Vibrational Frequencies calculated at B3LYP/STO-3G
| 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' |
3196 |
2852 |
10.30 |
|
|
|
| 2 |
A' |
1294 |
1155 |
82.58 |
|
|
|
| 3 |
A' |
1174 |
1047 |
85.26 |
|
|
|
| 4 |
A' |
744 |
664 |
98.46 |
|
|
|
| 5 |
A' |
554 |
495 |
12.10 |
|
|
|
| 6 |
A' |
374 |
333 |
0.86 |
|
|
|
| 7 |
A" |
1446 |
1291 |
60.25 |
|
|
|
| 8 |
A" |
1234 |
1101 |
51.82 |
|
|
|
| 9 |
A" |
318 |
284 |
3.82 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5166.4 cm
-1
Scaled (by 0.8924) Zero Point Vibrational Energy (zpe) 4610.5 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/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.189 |
|
|
|
| 2 |
H |
0.110 |
|
|
|
| 3 |
Cl |
-0.206 |
|
|
|
| 4 |
F |
-0.046 |
|
|
|
| 5 |
F |
-0.046 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.204 |
-0.795 |
0.000 |
2.343 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.951 |
-1.517 |
0.000 |
| y |
-1.517 |
-26.443 |
0.000 |
| z |
0.000 |
0.000 |
-26.034 |
|
| Traceless |
| | x | y | z |
| x |
1.287 |
-1.517 |
0.000 |
| y |
-1.517 |
-0.950 |
0.000 |
| z |
0.000 |
0.000 |
-0.337 |
|
| Polar |
| 3z2-r2 | -0.674 |
| x2-y2 | 1.491 |
| xy | -1.517 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.189 |
1.023 |
0.000 |
| y |
1.023 |
1.890 |
0.000 |
| z |
0.000 |
0.000 |
1.309 |
<r2> (average value of r
2) Å
2
| <r2> |
97.810 |
| (<r2>)1/2 |
9.890 |