Vibrational Frequencies calculated at PBEPBE/cc-pVDZ
| 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' |
3061 |
3043 |
7.51 |
|
|
|
| 2 |
A' |
1265 |
1257 |
18.04 |
|
|
|
| 3 |
A' |
1083 |
1077 |
203.77 |
|
|
|
| 4 |
A' |
702 |
698 |
46.85 |
|
|
|
| 5 |
A' |
439 |
437 |
1.81 |
|
|
|
| 6 |
A' |
264 |
262 |
0.08 |
|
|
|
| 7 |
A" |
1177 |
1171 |
52.21 |
|
|
|
| 8 |
A" |
738 |
734 |
277.10 |
|
|
|
| 9 |
A" |
350 |
348 |
0.58 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4539.8 cm
-1
Scaled (by 0.9942) Zero Point Vibrational Energy (zpe) 4513.5 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 PBEPBE/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.077 |
|
|
|
| 2 |
H |
0.119 |
|
|
|
| 3 |
F |
-0.111 |
|
|
|
| 4 |
Cl |
-0.042 |
|
|
|
| 5 |
Cl |
-0.042 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.000 |
0.745 |
0.000 |
1.247 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-35.397 |
-1.566 |
0.000 |
| y |
-1.566 |
-35.128 |
0.000 |
| z |
0.000 |
0.000 |
-36.162 |
|
| Traceless |
| | x | y | z |
| x |
0.248 |
-1.566 |
0.000 |
| y |
-1.566 |
0.652 |
0.000 |
| z |
0.000 |
0.000 |
-0.900 |
|
| Polar |
| 3z2-r2 | -1.799 |
| x2-y2 | -0.269 |
| xy | -1.566 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.142 |
0.175 |
0.000 |
| y |
0.175 |
4.224 |
0.000 |
| z |
0.000 |
0.000 |
6.500 |
<r2> (average value of r
2) Å
2
| <r2> |
133.850 |
| (<r2>)1/2 |
11.569 |