Vibrational Frequencies calculated at B3LYP/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' |
3115 |
3006 |
22.32 |
|
|
|
| 2 |
A' |
1318 |
1272 |
74.40 |
|
|
|
| 3 |
A' |
1141 |
1101 |
207.24 |
|
|
|
| 4 |
A' |
774 |
747 |
158.24 |
|
|
|
| 5 |
A' |
601 |
580 |
8.70 |
|
|
|
| 6 |
A' |
400 |
386 |
0.85 |
|
|
|
| 7 |
A" |
1395 |
1346 |
25.27 |
|
|
|
| 8 |
A" |
1180 |
1139 |
193.02 |
|
|
|
| 9 |
A" |
358 |
345 |
0.86 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5140.8 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 4960.9 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 B3LYP/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.145 |
|
|
|
| 2 |
H |
0.139 |
|
|
|
| 3 |
Cl |
-0.158 |
|
|
|
| 4 |
F |
-0.063 |
|
|
|
| 5 |
F |
-0.063 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.304 |
0.534 |
0.000 |
1.409 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.055 |
-0.983 |
0.000 |
| y |
-0.983 |
-28.556 |
0.000 |
| z |
0.000 |
0.000 |
-29.300 |
|
| Traceless |
| | x | y | z |
| x |
2.873 |
-0.983 |
0.000 |
| y |
-0.983 |
-0.879 |
0.000 |
| z |
0.000 |
0.000 |
-1.995 |
|
| Polar |
| 3z2-r2 | -3.989 |
| x2-y2 | 2.501 |
| xy | -0.983 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.216 |
0.835 |
0.000 |
| y |
0.835 |
3.814 |
0.000 |
| z |
0.000 |
0.000 |
3.266 |
<r2> (average value of r
2) Å
2
| <r2> |
91.086 |
| (<r2>)1/2 |
9.544 |