Vibrational Frequencies calculated at PBEPBE/6-311G*
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
3132 |
3099 |
1.46 |
|
|
|
| 2 |
A1 |
521 |
516 |
0.21 |
|
|
|
| 3 |
A1 |
216 |
214 |
0.00 |
|
|
|
| 4 |
E |
1138 |
1126 |
36.95 |
|
|
|
| 4 |
E |
1138 |
1126 |
36.93 |
|
|
|
| 5 |
E |
601 |
595 |
149.87 |
|
|
|
| 5 |
E |
601 |
595 |
149.89 |
|
|
|
| 6 |
E |
147 |
145 |
0.08 |
|
|
|
| 6 |
E |
147 |
145 |
0.08 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3820.2 cm
-1
Scaled (by 0.9896) Zero Point Vibrational Energy (zpe) 3780.5 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 PBEPBE/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.591 |
|
|
|
| 2 |
H |
0.342 |
|
|
|
| 3 |
Br |
0.083 |
|
|
|
| 4 |
Br |
0.083 |
|
|
|
| 5 |
Br |
0.083 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
0.968 |
0.968 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-60.474 |
0.000 |
0.000 |
| y |
0.000 |
-60.474 |
0.000 |
| z |
0.000 |
0.000 |
-59.659 |
|
| Traceless |
| | x | y | z |
| x |
-0.407 |
0.000 |
0.000 |
| y |
0.000 |
-0.407 |
0.000 |
| z |
0.000 |
0.000 |
0.815 |
|
| Polar |
| 3z2-r2 | 1.630 |
| x2-y2 | 0.000 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
10.770 |
0.000 |
0.000 |
| y |
0.000 |
10.770 |
-0.000 |
| z |
0.000 |
-0.000 |
5.459 |
<r2> (average value of r
2) Å
2
| <r2> |
409.283 |
| (<r2>)1/2 |
20.231 |