Vibrational Frequencies calculated at B3PW91/6-311+G(3df,2p)
| 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 |
3499 |
3349 |
264.79 |
28.63 |
0.23 |
0.38 |
| 2 |
Σ |
2348 |
2247 |
437.07 |
48.40 |
0.05 |
0.10 |
| 3 |
Σ |
1322 |
1266 |
133.01 |
23.83 |
0.20 |
0.34 |
| 4 |
Π |
576 |
552 |
2.16 |
0.27 |
0.75 |
0.86 |
| 4 |
Π |
576 |
552 |
2.16 |
0.27 |
0.75 |
0.86 |
| 5 |
Π |
247 |
236 |
73.64 |
5.17 |
0.75 |
0.86 |
| 5 |
Π |
247 |
236 |
73.64 |
5.17 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4407.3 cm
-1
Scaled (by 0.9573) Zero Point Vibrational Energy (zpe) 4219.1 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 B3PW91/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.642 |
|
|
|
| 2 |
N |
-0.067 |
|
|
|
| 3 |
C |
0.431 |
|
|
|
| 4 |
H |
0.278 |
|
|
|
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 |
-3.142 |
3.142 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.792 |
0.000 |
0.000 |
| y |
0.000 |
-16.792 |
0.000 |
| z |
0.000 |
0.000 |
-13.986 |
|
| Traceless |
| | x | y | z |
| x |
-1.403 |
0.000 |
0.000 |
| y |
0.000 |
-1.403 |
0.000 |
| z |
0.000 |
0.000 |
2.806 |
|
| Polar |
| 3z2-r2 | 5.611 |
| 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 |
2.396 |
0.000 |
0.000 |
| y |
0.000 |
2.396 |
0.000 |
| z |
0.000 |
0.000 |
6.300 |
<r2> (average value of r
2) Å
2
| <r2> |
34.197 |
| (<r2>)1/2 |
5.848 |