Vibrational Frequencies calculated at B3PW91/3-21G
| 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 |
3489 |
3353 |
74.78 |
|
|
|
| 2 |
Σ |
2394 |
2301 |
20.06 |
|
|
|
| 3 |
Σ |
2183 |
2099 |
1.00 |
|
|
|
| 4 |
Σ |
914 |
878 |
0.00 |
|
|
|
| 5 |
Π |
848 |
815 |
13.89 |
|
|
|
| 5 |
Π |
848 |
815 |
13.89 |
|
|
|
| 6 |
Π |
730 |
702 |
38.52 |
|
|
|
| 6 |
Π |
730 |
702 |
38.52 |
|
|
|
| 7 |
Π |
269 |
258 |
0.30 |
|
|
|
| 7 |
Π |
269 |
258 |
0.30 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6336.3 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 6090.5 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 B3PW91/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.484 |
|
|
|
| 2 |
C |
0.155 |
|
|
|
| 3 |
C |
0.257 |
|
|
|
| 4 |
C |
-0.250 |
|
|
|
| 5 |
H |
0.323 |
|
|
|
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 |
-3.634 |
3.634 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.506 |
0.000 |
0.000 |
| y |
0.000 |
-22.506 |
0.000 |
| z |
0.000 |
0.000 |
-20.254 |
|
| Traceless |
| | x | y | z |
| x |
-1.126 |
0.000 |
0.000 |
| y |
0.000 |
-1.126 |
0.000 |
| z |
0.000 |
0.000 |
2.251 |
|
| Polar |
| 3z2-r2 | 4.503 |
| 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 |
1.524 |
0.000 |
0.000 |
| y |
0.000 |
1.524 |
0.000 |
| z |
0.000 |
0.000 |
8.910 |
<r2> (average value of r
2) Å
2
| <r2> |
73.199 |
| (<r2>)1/2 |
8.556 |