Vibrational Frequencies calculated at ROHF/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 |
A' |
3376 |
3081 |
0.50 |
|
|
|
| 2 |
A' |
1356 |
1237 |
37.04 |
|
|
|
| 3 |
A' |
836 |
763 |
131.42 |
|
|
|
| 4 |
A' |
612 |
559 |
5.47 |
|
|
|
| 5 |
A' |
305 |
278 |
0.06 |
|
|
|
| 6 |
A' |
183 |
167 |
0.02 |
|
|
|
| 7 |
A" |
1302 |
1188 |
61.38 |
|
|
|
| 8 |
A" |
751 |
686 |
113.60 |
|
|
|
| 9 |
A" |
221 |
201 |
0.03 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4471.3 cm
-1
Scaled (by 0.9126) Zero Point Vibrational Energy (zpe) 4080.5 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 ROHF/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.308 |
|
|
|
| 2 |
H |
0.228 |
|
|
|
| 3 |
Cl |
-0.003 |
|
|
|
| 4 |
Br |
0.041 |
|
|
|
| 5 |
Br |
0.041 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.113 |
0.436 |
0.000 |
1.195 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-55.668 |
-1.488 |
0.000 |
| y |
-1.488 |
-55.592 |
0.000 |
| z |
0.000 |
0.000 |
-55.631 |
|
| Traceless |
| | x | y | z |
| x |
-0.057 |
-1.488 |
0.000 |
| y |
-1.488 |
0.057 |
0.000 |
| z |
0.000 |
0.000 |
-0.001 |
|
| Polar |
| 3z2-r2 | -0.001 |
| x2-y2 | -0.076 |
| xy | -1.488 |
| 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> |
0.000 |
| (<r2>)1/2 |
0.000 |