Vibrational Frequencies calculated at mPW1PW91/3-21G*
| 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' |
3126 |
2968 |
22.04 |
|
|
|
| 2 |
A' |
1570 |
1491 |
0.06 |
|
|
|
| 3 |
A' |
1418 |
1347 |
33.23 |
|
|
|
| 4 |
A' |
1110 |
1054 |
106.93 |
|
|
|
| 5 |
A' |
704 |
668 |
104.02 |
|
|
|
| 6 |
A' |
358 |
340 |
1.96 |
|
|
|
| 7 |
A" |
3196 |
3035 |
15.27 |
|
|
|
| 8 |
A" |
1272 |
1208 |
0.65 |
|
|
|
| 9 |
A" |
1034 |
982 |
0.19 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6893.5 cm
-1
Scaled (by 0.9496) Zero Point Vibrational Energy (zpe) 6546.1 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 mPW1PW91/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.195 |
|
|
|
| 2 |
F |
-0.279 |
|
|
|
| 3 |
Cl |
-0.049 |
|
|
|
| 4 |
H |
0.261 |
|
|
|
| 5 |
H |
0.261 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.043 |
1.836 |
0.000 |
2.112 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.218 |
-1.606 |
0.000 |
| y |
-1.606 |
-22.322 |
0.000 |
| z |
0.000 |
0.000 |
-23.174 |
|
| Traceless |
| | x | y | z |
| x |
-3.470 |
-1.606 |
0.000 |
| y |
-1.606 |
2.373 |
0.000 |
| z |
0.000 |
0.000 |
1.096 |
|
| Polar |
| 3z2-r2 | 2.192 |
| x2-y2 | -3.895 |
| xy | -1.606 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.715 |
0.741 |
0.000 |
| y |
0.741 |
3.724 |
0.000 |
| z |
0.000 |
0.000 |
2.192 |
<r2> (average value of r
2) Å
2
| <r2> |
67.091 |
| (<r2>)1/2 |
8.191 |