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' |
2991 |
2973 |
27.28 |
|
|
|
| 2 |
A' |
1425 |
1417 |
1.03 |
|
|
|
| 3 |
A' |
1297 |
1290 |
36.98 |
|
|
|
| 4 |
A' |
1074 |
1068 |
168.95 |
|
|
|
| 5 |
A' |
711 |
707 |
98.35 |
|
|
|
| 6 |
A' |
368 |
365 |
1.09 |
|
|
|
| 7 |
A" |
3071 |
3053 |
16.75 |
|
|
|
| 8 |
A" |
1193 |
1186 |
2.63 |
|
|
|
| 9 |
A" |
957 |
951 |
0.29 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6542.8 cm
-1
Scaled (by 0.9942) Zero Point Vibrational Energy (zpe) 6504.8 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 |
0.126 |
|
|
|
| 2 |
F |
-0.161 |
|
|
|
| 3 |
Cl |
-0.126 |
|
|
|
| 4 |
H |
0.081 |
|
|
|
| 5 |
H |
0.081 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.744 |
1.591 |
0.000 |
1.756 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.522 |
-1.288 |
0.000 |
| y |
-1.288 |
-22.360 |
0.000 |
| z |
0.000 |
0.000 |
-23.123 |
|
| Traceless |
| | x | y | z |
| x |
-2.780 |
-1.288 |
0.000 |
| y |
-1.288 |
1.963 |
0.000 |
| z |
0.000 |
0.000 |
0.818 |
|
| Polar |
| 3z2-r2 | 1.635 |
| x2-y2 | -3.162 |
| xy | -1.288 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.994 |
0.783 |
0.000 |
| y |
0.783 |
4.162 |
0.000 |
| z |
0.000 |
0.000 |
2.485 |
<r2> (average value of r
2) Å
2
| <r2> |
66.810 |
| (<r2>)1/2 |
8.174 |