Vibrational Frequencies calculated at PBEPBEultrafine/6-311G**
| 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 |
3081 |
3053 |
2.21 |
|
|
|
| 2 |
A |
1279 |
1267 |
13.37 |
|
|
|
| 3 |
A |
1145 |
1135 |
87.05 |
|
|
|
| 4 |
A |
1059 |
1049 |
215.43 |
|
|
|
| 5 |
A |
713 |
706 |
234.01 |
|
|
|
| 6 |
A |
554 |
549 |
68.56 |
|
|
|
| 7 |
A |
403 |
399 |
0.70 |
|
|
|
| 8 |
A |
255 |
253 |
1.02 |
|
|
|
| 9 |
A |
183 |
181 |
0.24 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4334.8 cm
-1
Scaled (by 0.9909) Zero Point Vibrational Energy (zpe) 4295.3 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 PBEPBEultrafine/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.132 |
|
|
|
| 2 |
H |
0.219 |
|
|
|
| 3 |
F |
-0.139 |
|
|
|
| 4 |
Cl |
-0.005 |
|
|
|
| 5 |
I |
0.058 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.064 |
0.053 |
1.223 |
1.226 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-51.429 |
0.481 |
1.923 |
| y |
0.481 |
-53.346 |
1.298 |
| z |
1.923 |
1.298 |
-50.969 |
|
| Traceless |
| | x | y | z |
| x |
0.729 |
0.481 |
1.923 |
| y |
0.481 |
-2.147 |
1.298 |
| z |
1.923 |
1.298 |
1.418 |
|
| Polar |
| 3z2-r2 | 2.837 |
| x2-y2 | 1.917 |
| xy | 0.481 |
| xz | 1.923 |
| yz | 1.298 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
10.773 |
-0.428 |
0.140 |
| y |
-0.428 |
6.178 |
0.364 |
| z |
0.140 |
0.364 |
4.970 |
<r2> (average value of r
2) Å
2
| <r2> |
237.365 |
| (<r2>)1/2 |
15.407 |