Vibrational Frequencies calculated at M06-2X/6-31G**
| 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' |
3145 |
2989 |
17.00 |
|
|
|
| 2 |
A' |
1519 |
1444 |
0.73 |
|
|
|
| 3 |
A' |
1357 |
1289 |
66.83 |
|
|
|
| 4 |
A' |
1174 |
1116 |
171.67 |
|
|
|
| 5 |
A' |
652 |
620 |
71.52 |
|
|
|
| 6 |
A' |
319 |
303 |
0.47 |
|
|
|
| 7 |
A" |
3231 |
3071 |
8.65 |
|
|
|
| 8 |
A" |
1267 |
1204 |
2.87 |
|
|
|
| 9 |
A" |
953 |
906 |
0.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6808.6 cm
-1
Scaled (by 0.9504) Zero Point Vibrational Energy (zpe) 6470.9 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 M06-2X/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.087 |
|
|
|
| 2 |
F |
-0.278 |
|
|
|
| 3 |
Br |
-0.141 |
|
|
|
| 4 |
H |
0.166 |
|
|
|
| 5 |
H |
0.166 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.680 |
-0.841 |
0.000 |
1.879 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-28.870 |
-3.083 |
0.000 |
| y |
-3.083 |
-29.412 |
0.000 |
| z |
0.000 |
0.000 |
-28.977 |
|
| Traceless |
| | x | y | z |
| x |
0.325 |
-3.083 |
0.000 |
| y |
-3.083 |
-0.488 |
0.000 |
| z |
0.000 |
0.000 |
0.164 |
|
| Polar |
| 3z2-r2 | 0.328 |
| x2-y2 | 0.542 |
| xy | -3.083 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.460 |
-0.462 |
0.000 |
| y |
-0.462 |
5.429 |
0.000 |
| z |
0.000 |
0.000 |
3.320 |
<r2> (average value of r
2) Å
2
| <r2> |
90.264 |
| (<r2>)1/2 |
9.501 |