Vibrational Frequencies calculated at ROHF/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' |
3403 |
3030 |
23.22 |
|
|
|
| 2 |
A' |
1451 |
1292 |
155.17 |
|
|
|
| 3 |
A' |
1245 |
1108 |
316.79 |
|
|
|
| 4 |
A' |
774 |
689 |
140.92 |
|
|
|
| 5 |
A' |
627 |
558 |
9.34 |
|
|
|
| 6 |
A' |
346 |
308 |
0.13 |
|
|
|
| 7 |
A" |
1542 |
1373 |
41.11 |
|
|
|
| 8 |
A" |
1310 |
1167 |
208.77 |
|
|
|
| 9 |
A" |
343 |
305 |
0.65 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5520.1 cm
-1
Scaled (by 0.8904) Zero Point Vibrational Energy (zpe) 4915.1 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 ROHF/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.601 |
|
|
|
| 2 |
H |
0.204 |
|
|
|
| 3 |
Br |
-0.145 |
|
|
|
| 4 |
F |
-0.330 |
|
|
|
| 5 |
F |
-0.330 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.560 |
-0.125 |
0.000 |
1.565 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.798 |
2.224 |
0.000 |
| y |
2.224 |
-33.946 |
0.000 |
| z |
0.000 |
0.000 |
-35.816 |
|
| Traceless |
| | x | y | z |
| x |
3.084 |
2.224 |
0.000 |
| y |
2.224 |
-0.139 |
0.000 |
| z |
0.000 |
0.000 |
-2.945 |
|
| Polar |
| 3z2-r2 | -5.889 |
| x2-y2 | 2.149 |
| xy | 2.224 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
123.787 |
| (<r2>)1/2 |
11.126 |