Vibrational Frequencies calculated at B1B95/6-31G**
| 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' |
3174 |
3031 |
7.53 |
|
|
|
| 2 |
A' |
1347 |
1286 |
24.74 |
|
|
|
| 3 |
A' |
1161 |
1109 |
190.13 |
|
|
|
| 4 |
A' |
744 |
711 |
48.41 |
|
|
|
| 5 |
A' |
459 |
439 |
2.33 |
|
|
|
| 6 |
A' |
278 |
265 |
0.28 |
|
|
|
| 7 |
A" |
1274 |
1217 |
65.93 |
|
|
|
| 8 |
A" |
798 |
762 |
275.39 |
|
|
|
| 9 |
A" |
367 |
350 |
0.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4801.3 cm
-1
Scaled (by 0.9548) Zero Point Vibrational Energy (zpe) 4584.3 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 B1B95/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.012 |
|
|
|
| 2 |
H |
0.210 |
|
|
|
| 3 |
F |
-0.225 |
|
|
|
| 4 |
Cl |
0.014 |
|
|
|
| 5 |
Cl |
0.014 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.129 |
0.790 |
0.000 |
1.378 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-35.349 |
-1.696 |
0.000 |
| y |
-1.696 |
-35.104 |
0.000 |
| z |
0.000 |
0.000 |
-36.302 |
|
| Traceless |
| | x | y | z |
| x |
0.353 |
-1.696 |
0.000 |
| y |
-1.696 |
0.722 |
0.000 |
| z |
0.000 |
0.000 |
-1.075 |
|
| Polar |
| 3z2-r2 | -2.151 |
| x2-y2 | -0.246 |
| xy | -1.696 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.185 |
0.130 |
0.000 |
| y |
0.130 |
4.110 |
0.000 |
| z |
0.000 |
0.000 |
6.240 |
<r2> (average value of r
2) Å
2
| <r2> |
131.038 |
| (<r2>)1/2 |
11.447 |