Vibrational Frequencies calculated at ROHF/aug-cc-pVDZ
| 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' |
3347 |
3347 |
7.96 |
|
|
|
| 2 |
A' |
1409 |
1409 |
109.59 |
|
|
|
| 3 |
A' |
1207 |
1207 |
308.48 |
|
|
|
| 4 |
A' |
774 |
774 |
132.02 |
|
|
|
| 5 |
A' |
621 |
621 |
6.77 |
|
|
|
| 6 |
A' |
350 |
350 |
0.09 |
|
|
|
| 7 |
A" |
1481 |
1481 |
16.24 |
|
|
|
| 8 |
A" |
1254 |
1254 |
223.20 |
|
|
|
| 9 |
A" |
341 |
341 |
0.26 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5391.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 5391.2 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-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.860 |
|
|
|
| 2 |
H |
-0.150 |
|
|
|
| 3 |
Br |
0.272 |
|
|
|
| 4 |
F |
-0.491 |
|
|
|
| 5 |
F |
-0.491 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.572 |
0.030 |
0.000 |
1.572 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.243 |
2.412 |
0.000 |
| y |
2.412 |
-34.727 |
0.000 |
| z |
0.000 |
0.000 |
-36.570 |
|
| Traceless |
| | x | y | z |
| x |
3.406 |
2.412 |
0.000 |
| y |
2.412 |
-0.320 |
0.000 |
| z |
0.000 |
0.000 |
-3.086 |
|
| Polar |
| 3z2-r2 | -6.171 |
| x2-y2 | 2.484 |
| xy | 2.412 |
| 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> |
124.353 |
| (<r2>)1/2 |
11.151 |