Vibrational Frequencies calculated at LSDA/6-31+G**
| 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' |
3109 |
3062 |
3.39 |
|
|
|
| 2 |
A' |
1144 |
1127 |
30.11 |
|
|
|
| 3 |
A' |
715 |
704 |
139.29 |
|
|
|
| 4 |
A' |
605 |
596 |
37.02 |
|
|
|
| 5 |
A' |
331 |
326 |
0.13 |
|
|
|
| 6 |
A' |
221 |
218 |
0.00 |
|
|
|
| 7 |
A" |
1187 |
1169 |
17.69 |
|
|
|
| 8 |
A" |
747 |
736 |
175.40 |
|
|
|
| 9 |
A" |
217 |
214 |
0.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4138.3 cm
-1
Scaled (by 0.985) Zero Point Vibrational Energy (zpe) 4076.2 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 LSDA/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.569 |
|
|
|
| 2 |
H |
0.301 |
|
|
|
| 3 |
Br |
0.011 |
|
|
|
| 4 |
Cl |
0.128 |
|
|
|
| 5 |
Cl |
0.128 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.898 |
0.686 |
0.000 |
1.130 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-47.732 |
-0.393 |
0.000 |
| y |
-0.393 |
-49.958 |
0.000 |
| z |
0.000 |
0.000 |
-50.474 |
|
| Traceless |
| | x | y | z |
| x |
2.484 |
-0.393 |
0.000 |
| y |
-0.393 |
-0.855 |
0.000 |
| z |
0.000 |
0.000 |
-1.629 |
|
| Polar |
| 3z2-r2 | -3.258 |
| x2-y2 | 2.226 |
| xy | -0.393 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.448 |
1.724 |
0.000 |
| y |
1.724 |
8.698 |
0.000 |
| z |
0.000 |
0.000 |
8.937 |
<r2> (average value of r
2) Å
2
| <r2> |
230.472 |
| (<r2>)1/2 |
15.181 |