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' |
3185 |
3090 |
1.23 |
|
|
|
| 2 |
A' |
1190 |
1154 |
24.00 |
|
|
|
| 3 |
A' |
720 |
699 |
143.59 |
|
|
|
| 4 |
A' |
556 |
539 |
9.83 |
|
|
|
| 5 |
A' |
275 |
267 |
0.07 |
|
|
|
| 6 |
A' |
164 |
159 |
0.01 |
|
|
|
| 7 |
A" |
1147 |
1113 |
42.48 |
|
|
|
| 8 |
A" |
629 |
610 |
141.60 |
|
|
|
| 9 |
A" |
197 |
191 |
0.06 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4031.2 cm
-1
Scaled (by 0.97) Zero Point Vibrational Energy (zpe) 3910.3 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 B3LYP/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.199 |
|
|
|
| 2 |
H |
0.148 |
|
|
|
| 3 |
Cl |
-0.000 |
|
|
|
| 4 |
Br |
0.026 |
|
|
|
| 5 |
Br |
0.026 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.908 |
0.435 |
0.000 |
1.007 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-54.233 |
-1.082 |
0.000 |
| y |
-1.082 |
-53.923 |
0.000 |
| z |
0.000 |
0.000 |
-53.990 |
|
| Traceless |
| | x | y | z |
| x |
-0.277 |
-1.082 |
0.000 |
| y |
-1.082 |
0.189 |
0.000 |
| z |
0.000 |
0.000 |
0.088 |
|
| Polar |
| 3z2-r2 | 0.176 |
| x2-y2 | -0.310 |
| xy | -1.082 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.627 |
1.544 |
0.000 |
| y |
1.544 |
7.516 |
0.000 |
| z |
0.000 |
0.000 |
9.547 |
<r2> (average value of r
2) Å
2
| <r2> |
0.000 |
| (<r2>)1/2 |
0.000 |