Vibrational Frequencies calculated at HF/6-311G**
| 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' |
3360 |
3052 |
27.21 |
|
|
|
| 2 |
A' |
1477 |
1342 |
125.21 |
|
|
|
| 3 |
A' |
1245 |
1131 |
303.25 |
|
|
|
| 4 |
A' |
884 |
804 |
182.84 |
|
|
|
| 5 |
A' |
655 |
595 |
11.07 |
|
|
|
| 6 |
A' |
452 |
411 |
0.47 |
|
|
|
| 7 |
A" |
1534 |
1393 |
44.04 |
|
|
|
| 8 |
A" |
1293 |
1175 |
268.31 |
|
|
|
| 9 |
A" |
402 |
365 |
1.48 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5650.6 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 5133.5 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 HF/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.508 |
|
|
|
| 2 |
H |
0.124 |
|
|
|
| 3 |
Cl |
-0.119 |
|
|
|
| 4 |
F |
-0.256 |
|
|
|
| 5 |
F |
-0.256 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.395 |
1.030 |
0.000 |
1.734 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.411 |
-1.251 |
0.000 |
| y |
-1.251 |
-29.459 |
0.000 |
| z |
0.000 |
0.000 |
-30.584 |
|
| Traceless |
| | x | y | z |
| x |
3.611 |
-1.251 |
0.000 |
| y |
-1.251 |
-0.962 |
0.000 |
| z |
0.000 |
0.000 |
-2.649 |
|
| Polar |
| 3z2-r2 | -5.298 |
| x2-y2 | 3.049 |
| xy | -1.251 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.454 |
0.925 |
0.000 |
| y |
0.925 |
2.948 |
0.000 |
| z |
0.000 |
0.000 |
2.308 |
<r2> (average value of r
2) Å
2
| <r2> |
89.358 |
| (<r2>)1/2 |
9.453 |