Vibrational Frequencies calculated at HF/Def2TZVPP
| 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' |
3322 |
3011 |
18.96 |
|
|
|
| 2 |
A' |
1467 |
1330 |
97.14 |
|
|
|
| 3 |
A' |
1245 |
1128 |
270.60 |
|
|
|
| 4 |
A' |
877 |
795 |
169.22 |
|
|
|
| 5 |
A' |
657 |
596 |
8.75 |
|
|
|
| 6 |
A' |
450 |
408 |
0.32 |
|
|
|
| 7 |
A" |
1523 |
1380 |
26.59 |
|
|
|
| 8 |
A" |
1288 |
1167 |
247.34 |
|
|
|
| 9 |
A" |
398 |
361 |
0.83 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5613.4 cm
-1
Scaled (by 0.9064) Zero Point Vibrational Energy (zpe) 5088.0 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/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.500 |
|
|
|
| 2 |
H |
0.057 |
|
|
|
| 3 |
Cl |
-0.100 |
|
|
|
| 4 |
F |
-0.228 |
|
|
|
| 5 |
F |
-0.228 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.217 |
1.008 |
0.000 |
1.580 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.049 |
-1.112 |
0.000 |
| y |
-1.112 |
-29.219 |
0.000 |
| z |
0.000 |
0.000 |
-30.230 |
|
| Traceless |
| | x | y | z |
| x |
3.676 |
-1.112 |
0.000 |
| y |
-1.112 |
-1.079 |
0.000 |
| z |
0.000 |
0.000 |
-2.597 |
|
| Polar |
| 3z2-r2 | -5.194 |
| x2-y2 | 3.170 |
| xy | -1.112 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.973 |
0.722 |
0.000 |
| y |
0.722 |
3.634 |
0.000 |
| z |
0.000 |
0.000 |
3.188 |
<r2> (average value of r
2) Å
2
| <r2> |
89.003 |
| (<r2>)1/2 |
9.434 |