Vibrational Frequencies calculated at BLYP/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' |
3050 |
3027 |
29.85 |
|
|
|
| 2 |
A' |
1277 |
1268 |
77.31 |
|
|
|
| 3 |
A' |
1079 |
1071 |
206.64 |
|
|
|
| 4 |
A' |
730 |
725 |
167.55 |
|
|
|
| 5 |
A' |
562 |
558 |
10.24 |
|
|
|
| 6 |
A' |
371 |
368 |
2.39 |
|
|
|
| 7 |
A" |
1348 |
1337 |
31.99 |
|
|
|
| 8 |
A" |
1111 |
1103 |
206.81 |
|
|
|
| 9 |
A" |
338 |
335 |
1.02 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4933.3 cm
-1
Scaled (by 0.9923) Zero Point Vibrational Energy (zpe) 4895.3 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 BLYP/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.341 |
|
|
|
| 2 |
H |
0.131 |
|
|
|
| 3 |
Cl |
-0.059 |
|
|
|
| 4 |
F |
-0.207 |
|
|
|
| 5 |
F |
-0.207 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.395 |
0.466 |
0.000 |
1.471 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.316 |
-1.018 |
0.000 |
| y |
-1.018 |
-28.604 |
0.000 |
| z |
0.000 |
0.000 |
-29.235 |
|
| Traceless |
| | x | y | z |
| x |
2.604 |
-1.018 |
0.000 |
| y |
-1.018 |
-0.829 |
0.000 |
| z |
0.000 |
0.000 |
-1.775 |
|
| Polar |
| 3z2-r2 | -3.550 |
| x2-y2 | 2.289 |
| xy | -1.018 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.947 |
1.028 |
0.000 |
| y |
1.028 |
3.465 |
0.000 |
| z |
0.000 |
0.000 |
2.795 |
<r2> (average value of r
2) Å
2
| <r2> |
93.792 |
| (<r2>)1/2 |
9.685 |