Vibrational Frequencies calculated at B2PLYP/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 |
2985 |
28.32 |
|
|
|
| 2 |
A' |
1556 |
1477 |
0.90 |
|
|
|
| 3 |
A' |
1426 |
1354 |
59.76 |
|
|
|
| 4 |
A' |
1125 |
1068 |
157.25 |
|
|
|
| 5 |
A' |
759 |
720 |
98.93 |
|
|
|
| 6 |
A' |
383 |
364 |
1.51 |
|
|
|
| 7 |
A" |
3223 |
3060 |
17.05 |
|
|
|
| 8 |
A" |
1281 |
1216 |
2.54 |
|
|
|
| 9 |
A" |
1043 |
990 |
0.78 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6970.6 cm
-1
Scaled (by 0.9492) Zero Point Vibrational Energy (zpe) 6616.5 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 B2PLYP/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.040 |
|
|
|
| 2 |
F |
-0.279 |
|
|
|
| 3 |
Cl |
-0.068 |
|
|
|
| 4 |
H |
0.194 |
|
|
|
| 5 |
H |
0.194 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.886 |
1.728 |
0.000 |
1.942 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.911 |
-1.424 |
0.000 |
| y |
-1.424 |
-22.416 |
0.000 |
| z |
0.000 |
0.000 |
-23.239 |
|
| Traceless |
| | x | y | z |
| x |
-3.083 |
-1.424 |
0.000 |
| y |
-1.424 |
2.159 |
0.000 |
| z |
0.000 |
0.000 |
0.925 |
|
| Polar |
| 3z2-r2 | 1.849 |
| x2-y2 | -3.494 |
| xy | -1.424 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.865 |
0.704 |
0.000 |
| y |
0.704 |
3.953 |
0.000 |
| z |
0.000 |
0.000 |
2.459 |
<r2> (average value of r
2) Å
2
| <r2> |
65.973 |
| (<r2>)1/2 |
8.122 |