Vibrational Frequencies calculated at PBEPBE/6-31+G**
| 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 |
3409 |
3371 |
92.55 |
|
|
|
| 2 |
Σ |
2287 |
2261 |
20.49 |
|
|
|
| 3 |
Σ |
2099 |
2076 |
0.00 |
|
|
|
| 4 |
Σ |
898 |
888 |
0.01 |
|
|
|
| 5 |
Π |
641 |
634 |
40.47 |
|
|
|
| 5 |
Π |
641 |
634 |
40.47 |
|
|
|
| 6 |
Π |
613 |
606 |
19.76 |
|
|
|
| 6 |
Π |
613 |
606 |
19.76 |
|
|
|
| 7 |
Π |
254 |
251 |
0.06 |
|
|
|
| 7 |
Π |
254 |
251 |
0.06 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5855.7 cm
-1
Scaled (by 0.9886) Zero Point Vibrational Energy (zpe) 5789.0 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/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.616 |
|
|
|
| 2 |
C |
-1.083 |
|
|
|
| 3 |
C |
1.336 |
|
|
|
| 4 |
C |
0.103 |
|
|
|
| 5 |
H |
0.260 |
|
|
|
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 |
-3.885 |
3.885 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.961 |
0.000 |
0.000 |
| y |
0.000 |
-22.961 |
0.000 |
| z |
0.000 |
0.000 |
-20.914 |
|
| Traceless |
| | x | y | z |
| x |
-1.023 |
0.000 |
0.000 |
| y |
0.000 |
-1.023 |
0.000 |
| z |
0.000 |
0.000 |
2.047 |
|
| Polar |
| 3z2-r2 | 4.094 |
| 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 |
2.792 |
0.000 |
0.000 |
| y |
0.000 |
2.792 |
0.000 |
| z |
0.000 |
0.000 |
11.145 |
<r2> (average value of r
2) Å
2
| <r2> |
74.628 |
| (<r2>)1/2 |
8.639 |