Vibrational Frequencies calculated at SVWN/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 |
Σ |
3410 |
3383 |
115.85 |
25.55 |
0.25 |
0.40 |
| 2 |
Σ |
2296 |
2278 |
145.95 |
85.28 |
0.03 |
0.05 |
| 3 |
Σ |
1104 |
1095 |
78.23 |
11.44 |
0.17 |
0.29 |
| 4 |
Π |
572 |
567 |
49.88 |
0.68 |
0.75 |
0.86 |
| 4 |
Π |
572 |
567 |
49.88 |
0.68 |
0.75 |
0.86 |
| 5 |
Π |
404 |
401 |
0.67 |
6.01 |
0.75 |
0.86 |
| 5 |
Π |
404 |
401 |
0.67 |
6.01 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4380.0 cm
-1
Scaled (by 0.9921) Zero Point Vibrational Energy (zpe) 4345.4 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 SVWN/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.448 |
|
|
|
| 2 |
C |
-0.608 |
|
|
|
| 3 |
F |
-0.211 |
|
|
|
| 4 |
H |
0.371 |
|
|
|
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 |
-0.483 |
0.483 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.179 |
0.000 |
0.000 |
| y |
0.000 |
-17.179 |
0.000 |
| z |
0.000 |
0.000 |
-12.944 |
|
| Traceless |
| | x | y | z |
| x |
-2.118 |
0.000 |
0.000 |
| y |
0.000 |
-2.118 |
0.000 |
| z |
0.000 |
0.000 |
4.235 |
|
| Polar |
| 3z2-r2 | 8.470 |
| 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 |
2.920 |
0.000 |
0.000 |
| y |
0.000 |
2.920 |
0.000 |
| z |
0.000 |
0.000 |
5.099 |
<r2> (average value of r
2) Å
2
| <r2> |
37.849 |
| (<r2>)1/2 |
6.152 |