Vibrational Frequencies calculated at BLYP/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' |
3020 |
3014 |
12.99 |
|
|
|
| 2 |
A' |
1403 |
1400 |
0.44 |
|
|
|
| 3 |
A' |
1254 |
1251 |
32.83 |
|
|
|
| 4 |
A' |
980 |
978 |
191.86 |
|
|
|
| 5 |
A' |
581 |
580 |
77.61 |
|
|
|
| 6 |
A' |
285 |
285 |
0.36 |
|
|
|
| 7 |
A" |
3115 |
3109 |
2.56 |
|
|
|
| 8 |
A" |
1177 |
1175 |
2.00 |
|
|
|
| 9 |
A" |
891 |
889 |
0.12 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6352.6 cm
-1
Scaled (by 0.9981) Zero Point Vibrational Energy (zpe) 6340.5 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 BLYP/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.761 |
|
|
|
| 2 |
F |
-0.332 |
|
|
|
| 3 |
Br |
0.158 |
|
|
|
| 4 |
H |
-0.294 |
|
|
|
| 5 |
H |
-0.294 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.681 |
-0.628 |
0.000 |
1.794 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-29.938 |
-3.395 |
0.000 |
| y |
-3.395 |
-30.642 |
0.000 |
| z |
0.000 |
0.000 |
-29.785 |
|
| Traceless |
| | x | y | z |
| x |
0.276 |
-3.395 |
0.000 |
| y |
-3.395 |
-0.780 |
0.000 |
| z |
0.000 |
0.000 |
0.505 |
|
| Polar |
| 3z2-r2 | 1.010 |
| x2-y2 | 0.704 |
| xy | -3.395 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.149 |
-0.295 |
0.000 |
| y |
-0.295 |
7.392 |
0.000 |
| z |
0.000 |
0.000 |
4.845 |
<r2> (average value of r
2) Å
2
| <r2> |
94.639 |
| (<r2>)1/2 |
9.728 |