Vibrational Frequencies calculated at PBE1PBE/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 |
A1 |
3237 |
3076 |
3.06 |
|
|
|
| 2 |
A1 |
547 |
520 |
0.91 |
|
|
|
| 3 |
A1 |
229 |
217 |
0.00 |
|
|
|
| 4 |
E |
1178 |
1119 |
35.44 |
|
|
|
| 4 |
E |
1178 |
1119 |
35.42 |
|
|
|
| 5 |
E |
669 |
635 |
107.97 |
|
|
|
| 5 |
E |
669 |
635 |
107.94 |
|
|
|
| 6 |
E |
161 |
153 |
0.00 |
|
|
|
| 6 |
E |
161 |
153 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4013.4 cm
-1
Scaled (by 0.9503) Zero Point Vibrational Energy (zpe) 3813.9 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 PBE1PBE/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.261 |
|
|
|
| 2 |
H |
0.291 |
|
|
|
| 3 |
Br |
-0.010 |
|
|
|
| 4 |
Br |
-0.010 |
|
|
|
| 5 |
Br |
-0.010 |
|
|
|
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 |
0.958 |
0.958 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-59.643 |
0.000 |
0.000 |
| y |
0.000 |
-59.643 |
0.000 |
| z |
0.000 |
0.000 |
-58.601 |
|
| Traceless |
| | x | y | z |
| x |
-0.521 |
0.000 |
0.000 |
| y |
0.000 |
-0.521 |
0.000 |
| z |
0.000 |
0.000 |
1.041 |
|
| Polar |
| 3z2-r2 | 2.083 |
| 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 |
10.215 |
0.000 |
0.000 |
| y |
0.000 |
10.215 |
-0.000 |
| z |
0.000 |
-0.000 |
6.058 |
<r2> (average value of r
2) Å
2
| <r2> |
395.471 |
| (<r2>)1/2 |
19.886 |