Vibrational Frequencies calculated at ROHF/aug-cc-pVTZ
| 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' |
3320 |
3320 |
9.99 |
|
|
|
| 2 |
A' |
1432 |
1432 |
112.99 |
|
|
|
| 3 |
A' |
1234 |
1234 |
318.53 |
|
|
|
| 4 |
A' |
776 |
776 |
138.16 |
|
|
|
| 5 |
A' |
640 |
640 |
7.57 |
|
|
|
| 6 |
A' |
352 |
352 |
0.08 |
|
|
|
| 7 |
A" |
1513 |
1513 |
19.69 |
|
|
|
| 8 |
A" |
1286 |
1286 |
221.95 |
|
|
|
| 9 |
A" |
342 |
342 |
0.29 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5447.7 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 5447.7 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-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.515 |
|
|
|
| 2 |
H |
0.301 |
|
|
|
| 3 |
Br |
-0.106 |
|
|
|
| 4 |
F |
-0.355 |
|
|
|
| 5 |
F |
-0.355 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.528 |
-0.055 |
0.000 |
1.529 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.153 |
2.332 |
0.000 |
| y |
2.332 |
-34.546 |
0.000 |
| z |
0.000 |
0.000 |
-36.314 |
|
| Traceless |
| | x | y | z |
| x |
3.277 |
2.332 |
0.000 |
| y |
2.332 |
-0.313 |
0.000 |
| z |
0.000 |
0.000 |
-2.964 |
|
| Polar |
| 3z2-r2 | -5.928 |
| x2-y2 | 2.393 |
| xy | 2.332 |
| 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> |
123.886 |
| (<r2>)1/2 |
11.130 |