Vibrational Frequencies calculated at B97D3/6-311G**
| 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 |
3427 |
3378 |
74.64 |
|
|
|
| 2 |
Σ |
2290 |
2257 |
18.21 |
|
|
|
| 3 |
Σ |
2103 |
2073 |
0.31 |
|
|
|
| 4 |
Σ |
893 |
881 |
0.00 |
|
|
|
| 5 |
Π |
656 |
646 |
40.18 |
|
|
|
| 5 |
Π |
656 |
646 |
40.18 |
|
|
|
| 6 |
Π |
540 |
532 |
2.78 |
|
|
|
| 6 |
Π |
540 |
532 |
2.78 |
|
|
|
| 7 |
Π |
233 |
230 |
0.13 |
|
|
|
| 7 |
Π |
233 |
230 |
0.13 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5785.0 cm
-1
Scaled (by 0.9857) Zero Point Vibrational Energy (zpe) 5702.3 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 B97D3/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.206 |
|
|
|
| 2 |
C |
-0.144 |
|
|
|
| 3 |
C |
0.271 |
|
|
|
| 4 |
C |
-0.046 |
|
|
|
| 5 |
H |
0.125 |
|
|
|
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 |
-3.749 |
3.749 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.490 |
0.000 |
0.000 |
| y |
0.000 |
-22.490 |
0.000 |
| z |
0.000 |
0.000 |
-20.502 |
|
| Traceless |
| | x | y | z |
| x |
-0.994 |
0.000 |
0.000 |
| y |
0.000 |
-0.994 |
0.000 |
| z |
0.000 |
0.000 |
1.987 |
|
| Polar |
| 3z2-r2 | 3.974 |
| 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 |
2.379 |
0.000 |
0.000 |
| y |
0.000 |
2.379 |
0.000 |
| z |
0.000 |
0.000 |
10.156 |
<r2> (average value of r
2) Å
2
| <r2> |
73.560 |
| (<r2>)1/2 |
8.577 |