Vibrational Frequencies calculated at B3LYP/3-21G
| 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' |
3211 |
3098 |
3.42 |
|
|
|
| 2 |
A' |
1329 |
1283 |
24.26 |
|
|
|
| 3 |
A' |
1149 |
1109 |
160.41 |
|
|
|
| 4 |
A' |
651 |
628 |
53.56 |
|
|
|
| 5 |
A' |
388 |
375 |
5.74 |
|
|
|
| 6 |
A' |
243 |
234 |
0.96 |
|
|
|
| 7 |
A" |
1228 |
1184 |
67.36 |
|
|
|
| 8 |
A" |
669 |
645 |
271.83 |
|
|
|
| 9 |
A" |
317 |
306 |
0.86 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4592.1 cm
-1
Scaled (by 0.9649) Zero Point Vibrational Energy (zpe) 4430.9 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 B3LYP/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.185 |
|
|
|
| 2 |
H |
0.306 |
|
|
|
| 3 |
F |
-0.218 |
|
|
|
| 4 |
Cl |
0.048 |
|
|
|
| 5 |
Cl |
0.048 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.250 |
1.359 |
0.000 |
1.846 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-35.997 |
-1.939 |
0.000 |
| y |
-1.939 |
-35.935 |
0.000 |
| z |
0.000 |
0.000 |
-38.683 |
|
| Traceless |
| | x | y | z |
| x |
1.312 |
-1.939 |
0.000 |
| y |
-1.939 |
1.405 |
0.000 |
| z |
0.000 |
0.000 |
-2.718 |
|
| Polar |
| 3z2-r2 | -5.435 |
| x2-y2 | -0.062 |
| xy | -1.939 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.314 |
0.239 |
0.000 |
| y |
0.239 |
3.702 |
0.000 |
| z |
0.000 |
0.000 |
6.498 |
<r2> (average value of r
2) Å
2
| <r2> |
142.474 |
| (<r2>)1/2 |
11.936 |