Vibrational Frequencies calculated at HSEh1PBE/6-311G**
| 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 |
3513 |
3374 |
101.09 |
21.24 |
0.26 |
0.41 |
| 2 |
Σ |
2353 |
2260 |
129.91 |
40.41 |
0.19 |
0.32 |
| 3 |
Σ |
1099 |
1055 |
86.80 |
8.03 |
0.23 |
0.37 |
| 4 |
Π |
630 |
605 |
52.86 |
1.23 |
0.75 |
0.86 |
| 4 |
Π |
630 |
605 |
52.86 |
1.23 |
0.75 |
0.86 |
| 5 |
Π |
441 |
424 |
1.87 |
12.19 |
0.75 |
0.86 |
| 5 |
Π |
441 |
424 |
1.87 |
12.19 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4553.5 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 4373.1 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 HSEh1PBE/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.123 |
|
|
|
| 2 |
C |
-0.132 |
|
|
|
| 3 |
F |
-0.128 |
|
|
|
| 4 |
H |
0.137 |
|
|
|
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 |
-0.565 |
0.565 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.835 |
0.000 |
0.000 |
| y |
0.000 |
-16.835 |
0.000 |
| z |
0.000 |
0.000 |
-12.764 |
|
| Traceless |
| | x | y | z |
| x |
-2.035 |
0.000 |
0.000 |
| y |
0.000 |
-2.035 |
0.000 |
| z |
0.000 |
0.000 |
4.071 |
|
| Polar |
| 3z2-r2 | 8.141 |
| 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 |
1.560 |
0.000 |
0.000 |
| y |
0.000 |
1.560 |
0.000 |
| z |
0.000 |
0.000 |
4.488 |
<r2> (average value of r
2) Å
2
| <r2> |
37.669 |
| (<r2>)1/2 |
6.138 |