Vibrational Frequencies calculated at PBEPBE/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 |
3435 |
3388 |
74.27 |
|
|
|
| 2 |
Σ |
2281 |
2250 |
27.88 |
|
|
|
| 3 |
Σ |
2082 |
2053 |
0.00 |
|
|
|
| 4 |
Σ |
899 |
887 |
0.00 |
|
|
|
| 5 |
Π |
654 |
645 |
58.20 |
|
|
|
| 5 |
Π |
654 |
645 |
58.20 |
|
|
|
| 6 |
Π |
562 |
554 |
0.50 |
|
|
|
| 6 |
Π |
562 |
554 |
0.50 |
|
|
|
| 7 |
Π |
236 |
233 |
0.01 |
|
|
|
| 7 |
Π |
236 |
233 |
0.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5800.6 cm
-1
Scaled (by 0.9862) Zero Point Vibrational Energy (zpe) 5720.5 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 PBEPBE/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.174 |
|
|
|
| 2 |
C |
-0.079 |
|
|
|
| 3 |
C |
0.342 |
|
|
|
| 4 |
C |
-0.374 |
|
|
|
| 5 |
H |
0.286 |
|
|
|
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 |
-3.817 |
3.817 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.212 |
0.000 |
0.000 |
| y |
0.000 |
-22.212 |
0.000 |
| z |
0.000 |
0.000 |
-20.764 |
|
| Traceless |
| | x | y | z |
| x |
-0.724 |
0.000 |
0.000 |
| y |
0.000 |
-0.724 |
0.000 |
| z |
0.000 |
0.000 |
1.448 |
|
| Polar |
| 3z2-r2 | 2.897 |
| 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 |
1.798 |
0.000 |
0.000 |
| y |
0.000 |
1.798 |
0.000 |
| z |
0.000 |
0.000 |
9.954 |
<r2> (average value of r
2) Å
2
| <r2> |
74.556 |
| (<r2>)1/2 |
8.635 |