Vibrational Frequencies calculated at B3LYP/aug-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 |
A1 |
1952 |
1894 |
462.41 |
10.79 |
0.16 |
0.27 |
| 2 |
A1 |
945 |
917 |
59.13 |
8.38 |
0.06 |
0.11 |
| 3 |
A1 |
562 |
546 |
4.80 |
0.99 |
0.74 |
0.85 |
| 4 |
B1 |
766 |
744 |
34.34 |
0.45 |
0.75 |
0.86 |
| 5 |
B2 |
1203 |
1167 |
418.04 |
1.53 |
0.75 |
0.86 |
| 6 |
B2 |
602 |
584 |
5.86 |
1.82 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 3015.1 cm
-1
Scaled (by 0.9704) Zero Point Vibrational Energy (zpe) 2925.8 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 B3LYP/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.274 |
|
|
|
| 2 |
C |
0.904 |
|
|
|
| 3 |
F |
-0.315 |
|
|
|
| 4 |
F |
-0.315 |
|
|
|
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 |
-1.001 |
1.001 |
| CHELPG |
0.000 |
0.000 |
0.000 |
0.000 |
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.015 |
0.000 |
0.000 |
| y |
0.000 |
-21.389 |
0.000 |
| z |
0.000 |
0.000 |
-23.361 |
|
| Traceless |
| | x | y | z |
| x |
3.360 |
0.000 |
0.000 |
| y |
0.000 |
-0.201 |
0.000 |
| z |
0.000 |
0.000 |
-3.159 |
|
| Polar |
| 3z2-r2 | -6.318 |
| x2-y2 | 2.374 |
| 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 |
1.981 |
0.000 |
0.000 |
| y |
0.000 |
2.826 |
0.000 |
| z |
0.000 |
0.000 |
3.387 |
<r2> (average value of r
2) Å
2
| <r2> |
55.410 |
| (<r2>)1/2 |
7.444 |