Vibrational Frequencies calculated at B1B95/6-31G*
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Σ |
3542 |
3362 |
86.01 |
26.44 |
0.20 |
0.34 |
| 2 |
Σ |
2375 |
2254 |
106.04 |
31.04 |
0.25 |
0.40 |
| 3 |
Σ |
1113 |
1056 |
75.59 |
8.61 |
0.23 |
0.38 |
| 4 |
Π |
614 |
583 |
45.39 |
0.04 |
0.75 |
0.86 |
| 4 |
Π |
614 |
583 |
45.39 |
0.04 |
0.75 |
0.86 |
| 5 |
Π |
405 |
384 |
4.09 |
11.55 |
0.75 |
0.86 |
| 5 |
Π |
405 |
384 |
4.09 |
11.55 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4533.4 cm
-1
Scaled (by 0.9493) Zero Point Vibrational Energy (zpe) 4303.6 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 B1B95/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.112 |
|
|
|
| 2 |
C |
-0.145 |
|
|
|
| 3 |
F |
-0.185 |
|
|
|
| 4 |
H |
0.218 |
|
|
|
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 |
-0.568 |
0.568 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.353 |
0.000 |
0.000 |
| y |
0.000 |
-16.353 |
0.000 |
| z |
0.000 |
0.000 |
-12.359 |
|
| Traceless |
| | x | y | z |
| x |
-1.997 |
0.000 |
0.000 |
| y |
0.000 |
-1.997 |
0.000 |
| z |
0.000 |
0.000 |
3.995 |
|
| Polar |
| 3z2-r2 | 7.990 |
| 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 |
1.313 |
0.000 |
0.000 |
| y |
0.000 |
1.313 |
0.000 |
| z |
0.000 |
0.000 |
4.353 |
<r2> (average value of r
2) Å
2
| <r2> |
37.623 |
| (<r2>)1/2 |
6.134 |