Vibrational Frequencies calculated at B3LYP/CEP-121G*
| 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' |
3141 |
3045 |
26.09 |
|
|
|
| 2 |
A' |
1326 |
1285 |
92.91 |
|
|
|
| 3 |
A' |
1103 |
1069 |
244.65 |
|
|
|
| 4 |
A' |
788 |
764 |
161.39 |
|
|
|
| 5 |
A' |
581 |
563 |
7.01 |
|
|
|
| 6 |
A' |
397 |
385 |
0.13 |
|
|
|
| 7 |
A" |
1374 |
1332 |
25.59 |
|
|
|
| 8 |
A" |
1125 |
1091 |
249.92 |
|
|
|
| 9 |
A" |
352 |
342 |
0.83 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5093.9 cm
-1
Scaled (by 0.9694) Zero Point Vibrational Energy (zpe) 4938.0 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/CEP-121G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.263 |
|
|
|
| 2 |
H |
0.181 |
|
|
|
| 3 |
Cl |
-0.079 |
|
|
|
| 4 |
F |
-0.182 |
|
|
|
| 5 |
F |
-0.182 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.201 |
0.986 |
0.000 |
1.554 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.543 |
-1.041 |
0.000 |
| y |
-1.041 |
-28.531 |
0.000 |
| z |
0.000 |
0.000 |
-29.525 |
|
| Traceless |
| | x | y | z |
| x |
3.485 |
-1.041 |
0.000 |
| y |
-1.041 |
-0.997 |
0.000 |
| z |
0.000 |
0.000 |
-2.488 |
|
| Polar |
| 3z2-r2 | -4.976 |
| x2-y2 | 2.988 |
| xy | -1.041 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.067 |
0.954 |
0.000 |
| y |
0.954 |
3.679 |
0.000 |
| z |
0.000 |
0.000 |
3.014 |
<r2> (average value of r
2) Å
2
| <r2> |
0.000 |
| (<r2>)1/2 |
0.000 |