Vibrational Frequencies calculated at B2PLYP=FULLultrafine/6-31G*
| 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' |
3172 |
3010 |
39.32 |
81.38 |
0.26 |
0.41 |
| 2 |
A' |
1195 |
1134 |
83.52 |
5.51 |
0.11 |
0.20 |
| 3 |
A' |
1052 |
998 |
12.61 |
4.96 |
0.56 |
0.71 |
| 4 |
A' |
539 |
511 |
4.41 |
1.51 |
0.74 |
0.85 |
| 5 |
A" |
1391 |
1320 |
88.78 |
4.35 |
0.75 |
0.86 |
| 6 |
A" |
1218 |
1156 |
183.14 |
5.64 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4283.8 cm
-1
Scaled (by 0.9487) Zero Point Vibrational Energy (zpe) 4064.0 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/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.349 |
|
|
|
| 2 |
H |
0.148 |
|
|
|
| 3 |
F |
-0.248 |
|
|
|
| 4 |
F |
-0.248 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.646 |
1.120 |
0.000 |
1.293 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.012 |
-0.803 |
-0.000 |
| y |
-0.803 |
-14.454 |
0.001 |
| z |
-0.000 |
0.001 |
-16.961 |
|
| Traceless |
| | x | y | z |
| x |
0.696 |
-0.803 |
-0.000 |
| y |
-0.803 |
1.532 |
0.001 |
| z |
-0.000 |
0.001 |
-2.228 |
|
| Polar |
| 3z2-r2 | -4.456 |
| x2-y2 | -0.558 |
| xy | -0.803 |
| xz | -0.000 |
| yz | 0.001 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.400 |
-0.286 |
0.000 |
| y |
-0.286 |
1.779 |
0.001 |
| z |
0.000 |
0.001 |
2.023 |
<r2> (average value of r
2) Å
2
| <r2> |
36.371 |
| (<r2>)1/2 |
6.031 |