Vibrational Frequencies calculated at ROHF/aug-cc-pVQZ
| 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' |
3319 |
3319 |
10.34 |
|
|
|
| 2 |
A' |
1434 |
1434 |
113.00 |
|
|
|
| 3 |
A' |
1232 |
1232 |
319.09 |
|
|
|
| 4 |
A' |
777 |
777 |
138.48 |
|
|
|
| 5 |
A' |
642 |
642 |
7.49 |
|
|
|
| 6 |
A' |
352 |
352 |
0.08 |
|
|
|
| 7 |
A" |
1516 |
1516 |
18.84 |
|
|
|
| 8 |
A" |
1283 |
1283 |
222.59 |
|
|
|
| 9 |
A" |
343 |
343 |
0.29 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5448.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 5448.1 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/aug-cc-pVQZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.701 |
|
|
|
| 2 |
H |
0.343 |
|
|
|
| 3 |
Br |
0.042 |
|
|
|
| 4 |
F |
-0.543 |
|
|
|
| 5 |
F |
-0.543 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.518 |
-0.062 |
0.000 |
1.520 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.140 |
2.307 |
0.000 |
| y |
2.307 |
-34.512 |
0.000 |
| z |
0.000 |
0.000 |
-36.256 |
|
| Traceless |
| | x | y | z |
| x |
3.244 |
2.307 |
0.000 |
| y |
2.307 |
-0.314 |
0.000 |
| z |
0.000 |
0.000 |
-2.930 |
|
| Polar |
| 3z2-r2 | -5.860 |
| x2-y2 | 2.372 |
| xy | 2.307 |
| 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> |
123.730 |
| (<r2>)1/2 |
11.123 |