Vibrational Frequencies calculated at PBEPBEultrafine/cc-pCVTZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Σ |
3414 |
3414 |
93.00 |
26.60 |
0.24 |
0.38 |
| 2 |
Σ |
2259 |
2259 |
126.28 |
45.46 |
0.13 |
0.23 |
| 3 |
Σ |
1065 |
1065 |
72.26 |
9.49 |
0.21 |
0.35 |
| 4 |
Π |
566 |
566 |
46.70 |
0.21 |
0.75 |
0.86 |
| 4 |
Π |
566 |
566 |
46.70 |
0.21 |
0.75 |
0.86 |
| 5 |
Π |
374 |
374 |
3.16 |
9.56 |
0.75 |
0.86 |
| 5 |
Π |
374 |
374 |
3.16 |
9.56 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4309.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4309.4 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 PBEPBEultrafine/cc-pCVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.162 |
|
|
|
| 2 |
C |
-0.281 |
|
|
|
| 3 |
F |
-0.047 |
|
|
|
| 4 |
H |
0.165 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-0.425 |
0.425 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.014 |
0.000 |
0.000 |
| y |
0.000 |
-17.014 |
0.000 |
| z |
0.000 |
0.000 |
-12.764 |
|
| Traceless |
| | x | y | z |
| x |
-2.125 |
0.000 |
0.000 |
| y |
0.000 |
-2.125 |
0.000 |
| z |
0.000 |
0.000 |
4.250 |
|
| Polar |
| 3z2-r2 | 8.500 |
| x2-y2 | 0.000 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.158 |
0.000 |
0.000 |
| y |
0.000 |
2.158 |
0.000 |
| z |
0.000 |
0.000 |
4.866 |
<r2> (average value of r
2) Å
2
| <r2> |
38.207 |
| (<r2>)1/2 |
6.181 |