Vibrational Frequencies calculated at BLYP/6-31G(2df,p)
| 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' |
2991 |
2974 |
24.89 |
|
|
|
| 2 |
A' |
1468 |
1460 |
0.75 |
|
|
|
| 3 |
A' |
1326 |
1318 |
42.37 |
|
|
|
| 4 |
A' |
1073 |
1067 |
148.93 |
|
|
|
| 5 |
A' |
676 |
672 |
98.26 |
|
|
|
| 6 |
A' |
358 |
356 |
1.28 |
|
|
|
| 7 |
A" |
3065 |
3048 |
16.29 |
|
|
|
| 8 |
A" |
1214 |
1207 |
2.67 |
|
|
|
| 9 |
A" |
971 |
966 |
0.31 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6569.9 cm
-1
Scaled (by 0.9945) Zero Point Vibrational Energy (zpe) 6533.8 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/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.050 |
|
|
|
| 2 |
F |
-0.064 |
|
|
|
| 3 |
Cl |
-0.167 |
|
|
|
| 4 |
H |
0.140 |
|
|
|
| 5 |
H |
0.140 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.593 |
1.702 |
0.000 |
1.803 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.626 |
-1.250 |
0.000 |
| y |
-1.250 |
-22.314 |
0.000 |
| z |
0.000 |
0.000 |
-23.131 |
|
| Traceless |
| | x | y | z |
| x |
-2.904 |
-1.250 |
0.000 |
| y |
-1.250 |
2.065 |
0.000 |
| z |
0.000 |
0.000 |
0.839 |
|
| Polar |
| 3z2-r2 | 1.678 |
| x2-y2 | -3.313 |
| xy | -1.250 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.561 |
0.706 |
0.000 |
| y |
0.706 |
4.569 |
0.000 |
| z |
0.000 |
0.000 |
3.094 |
<r2> (average value of r
2) Å
2
| <r2> |
67.293 |
| (<r2>)1/2 |
8.203 |