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 |
3506 |
3364 |
85.97 |
21.10 |
0.27 |
0.42 |
| 2 |
Σ |
2354 |
2259 |
128.81 |
39.66 |
0.19 |
0.33 |
| 3 |
Σ |
1098 |
1054 |
86.83 |
7.97 |
0.23 |
0.38 |
| 4 |
Π |
607 |
582 |
54.10 |
1.04 |
0.75 |
0.86 |
| 4 |
Π |
607 |
582 |
54.10 |
1.04 |
0.75 |
0.86 |
| 5 |
Π |
436 |
418 |
3.36 |
12.81 |
0.75 |
0.86 |
| 5 |
Π |
436 |
418 |
3.36 |
12.81 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4521.0 cm
-1
Scaled (by 0.9596) Zero Point Vibrational Energy (zpe) 4338.3 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 HSEh1PBE/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.124 |
|
|
|
| 2 |
C |
-0.253 |
|
|
|
| 3 |
F |
-0.130 |
|
|
|
| 4 |
H |
0.258 |
|
|
|
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 |
-0.590 |
0.590 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.871 |
0.000 |
0.000 |
| y |
0.000 |
-16.871 |
0.000 |
| z |
0.000 |
0.000 |
-12.655 |
|
| Traceless |
| | x | y | z |
| x |
-2.108 |
0.000 |
0.000 |
| y |
0.000 |
-2.108 |
0.000 |
| z |
0.000 |
0.000 |
4.216 |
|
| Polar |
| 3z2-r2 | 8.432 |
| 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 |
1.545 |
0.000 |
0.000 |
| y |
0.000 |
1.545 |
0.000 |
| z |
0.000 |
0.000 |
4.457 |
<r2> (average value of r
2) Å
2
| <r2> |
37.671 |
| (<r2>)1/2 |
6.138 |