Vibrational Frequencies calculated at BLYP/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' |
3066 |
3042 |
5.41 |
|
|
|
| 2 |
A' |
1420 |
1409 |
0.55 |
|
|
|
| 3 |
A' |
1212 |
1203 |
61.25 |
|
|
|
| 4 |
A' |
669 |
664 |
105.58 |
|
|
|
| 5 |
A' |
556 |
551 |
55.50 |
|
|
|
| 6 |
A' |
215 |
213 |
0.20 |
|
|
|
| 7 |
A" |
3156 |
3132 |
0.08 |
|
|
|
| 8 |
A" |
1109 |
1100 |
0.00 |
|
|
|
| 9 |
A" |
824 |
818 |
3.23 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6112.9 cm
-1
Scaled (by 0.9923) Zero Point Vibrational Energy (zpe) 6065.9 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 BLYP/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.279 |
|
|
|
| 2 |
Br |
-0.077 |
|
|
|
| 3 |
Cl |
-0.018 |
|
|
|
| 4 |
H |
0.187 |
|
|
|
| 5 |
H |
0.187 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.926 |
1.380 |
0.000 |
1.661 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-38.977 |
1.263 |
0.000 |
| y |
1.263 |
-34.740 |
0.000 |
| z |
0.000 |
0.000 |
-36.963 |
|
| Traceless |
| | x | y | z |
| x |
-3.126 |
1.263 |
0.000 |
| y |
1.263 |
3.230 |
0.000 |
| z |
0.000 |
0.000 |
-0.104 |
|
| Polar |
| 3z2-r2 | -0.209 |
| x2-y2 | -4.237 |
| xy | 1.263 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.042 |
-1.612 |
0.000 |
| y |
-1.612 |
5.859 |
0.000 |
| z |
0.000 |
0.000 |
3.880 |
<r2> (average value of r
2) Å
2
| <r2> |
153.172 |
| (<r2>)1/2 |
12.376 |