Vibrational Frequencies calculated at B3LYPultrafine/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' |
3104 |
2973 |
28.99 |
|
|
|
| 2 |
A' |
1536 |
1472 |
0.89 |
|
|
|
| 3 |
A' |
1402 |
1343 |
58.13 |
|
|
|
| 4 |
A' |
1121 |
1074 |
162.08 |
|
|
|
| 5 |
A' |
729 |
699 |
103.38 |
|
|
|
| 6 |
A' |
377 |
361 |
1.44 |
|
|
|
| 7 |
A" |
3178 |
3044 |
18.99 |
|
|
|
| 8 |
A" |
1266 |
1213 |
2.60 |
|
|
|
| 9 |
A" |
1024 |
981 |
0.57 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6867.7 cm
-1
Scaled (by 0.958) Zero Point Vibrational Energy (zpe) 6579.3 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 B3LYPultrafine/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.049 |
|
|
|
| 2 |
F |
-0.259 |
|
|
|
| 3 |
Cl |
-0.072 |
|
|
|
| 4 |
H |
0.190 |
|
|
|
| 5 |
H |
0.190 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.804 |
1.758 |
0.000 |
1.933 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.718 |
-1.400 |
0.000 |
| y |
-1.400 |
-22.348 |
0.000 |
| z |
0.000 |
0.000 |
-23.146 |
|
| Traceless |
| | x | y | z |
| x |
-2.972 |
-1.400 |
0.000 |
| y |
-1.400 |
2.084 |
0.000 |
| z |
0.000 |
0.000 |
0.887 |
|
| Polar |
| 3z2-r2 | 1.775 |
| x2-y2 | -3.371 |
| xy | -1.400 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.897 |
0.723 |
0.000 |
| y |
0.723 |
4.032 |
0.000 |
| z |
0.000 |
0.000 |
2.486 |
<r2> (average value of r
2) Å
2
| <r2> |
66.361 |
| (<r2>)1/2 |
8.146 |