Vibrational Frequencies calculated at B2PLYP=FULLultrafine/aug-cc-pVTZ
| 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 |
1954 |
1874 |
457.88 |
12.04 |
0.13 |
0.23 |
| 2 |
A1 |
967 |
927 |
60.85 |
9.14 |
0.05 |
0.10 |
| 3 |
A1 |
581 |
557 |
5.47 |
0.90 |
0.75 |
0.85 |
| 4 |
B1 |
780 |
748 |
34.50 |
0.44 |
0.75 |
0.86 |
| 5 |
B2 |
1232 |
1182 |
420.19 |
1.40 |
0.75 |
0.86 |
| 6 |
B2 |
617 |
591 |
6.34 |
1.67 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 3064.6 cm
-1
Scaled (by 0.9591) Zero Point Vibrational Energy (zpe) 2939.3 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 B2PLYP=FULLultrafine/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.276 |
|
|
|
| 2 |
C |
0.640 |
|
|
|
| 3 |
F |
-0.182 |
|
|
|
| 4 |
F |
-0.182 |
|
|
|
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 |
-1.015 |
1.015 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-18.968 |
0.000 |
0.000 |
| y |
0.000 |
-21.353 |
0.000 |
| z |
0.000 |
0.000 |
-23.257 |
|
| Traceless |
| | x | y | z |
| x |
3.337 |
0.000 |
0.000 |
| y |
0.000 |
-0.240 |
0.000 |
| z |
0.000 |
0.000 |
-3.097 |
|
| Polar |
| 3z2-r2 | -6.194 |
| x2-y2 | 2.385 |
| 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 |
2.057 |
0.000 |
0.000 |
| y |
0.000 |
2.853 |
0.000 |
| z |
0.000 |
0.000 |
3.405 |
<r2> (average value of r
2) Å
2
| <r2> |
54.775 |
| (<r2>)1/2 |
7.401 |