Vibrational Frequencies calculated at B3LYP/cc-pVDZ
| 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' |
3180 |
3085 |
0.33 |
|
|
|
| 2 |
A' |
1171 |
1136 |
37.82 |
|
|
|
| 3 |
A' |
696 |
675 |
136.34 |
|
|
|
| 4 |
A' |
587 |
569 |
34.44 |
|
|
|
| 5 |
A' |
325 |
315 |
0.21 |
|
|
|
| 6 |
A' |
217 |
210 |
0.09 |
|
|
|
| 7 |
A" |
1211 |
1174 |
20.96 |
|
|
|
| 8 |
A" |
736 |
714 |
166.93 |
|
|
|
| 9 |
A" |
212 |
205 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4166.7 cm
-1
Scaled (by 0.97) Zero Point Vibrational Energy (zpe) 4041.7 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/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.161 |
|
|
|
| 2 |
H |
0.148 |
|
|
|
| 3 |
Br |
0.020 |
|
|
|
| 4 |
Cl |
-0.004 |
|
|
|
| 5 |
Cl |
-0.004 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.865 |
0.647 |
0.000 |
1.081 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-47.104 |
-0.293 |
0.000 |
| y |
-0.293 |
-49.076 |
0.000 |
| z |
0.000 |
0.000 |
-49.555 |
|
| Traceless |
| | x | y | z |
| x |
2.211 |
-0.293 |
0.000 |
| y |
-0.293 |
-0.746 |
0.000 |
| z |
0.000 |
0.000 |
-1.465 |
|
| Polar |
| 3z2-r2 | -2.929 |
| x2-y2 | 1.972 |
| xy | -0.293 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.634 |
1.953 |
0.000 |
| y |
1.953 |
7.135 |
0.000 |
| z |
0.000 |
0.000 |
7.420 |
<r2> (average value of r
2) Å
2
| <r2> |
238.640 |
| (<r2>)1/2 |
15.448 |