Vibrational Frequencies calculated at PBE1PBE/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 |
A' |
1927 |
1831 |
374.67 |
|
|
|
| 2 |
A' |
1418 |
1348 |
220.35 |
|
|
|
| 3 |
A' |
1067 |
1014 |
30.11 |
|
|
|
| 4 |
A' |
850 |
808 |
162.11 |
|
|
|
| 5 |
A' |
698 |
663 |
1.47 |
|
|
|
| 6 |
A' |
507 |
482 |
16.91 |
|
|
|
| 7 |
A' |
327 |
311 |
1.54 |
|
|
|
| 8 |
A" |
746 |
709 |
14.76 |
|
|
|
| 9 |
A" |
171 |
163 |
0.12 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3855.3 cm
-1
Scaled (by 0.9503) Zero Point Vibrational Energy (zpe) 3663.7 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 PBE1PBE/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
0.776 |
|
|
|
| 2 |
O |
-0.036 |
|
|
|
| 3 |
O |
-0.315 |
|
|
|
| 4 |
O |
-0.317 |
|
|
|
| 5 |
F |
-0.107 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.057 |
-0.261 |
0.000 |
0.267 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-27.267 |
0.309 |
0.000 |
| y |
0.309 |
-26.815 |
0.000 |
| z |
0.000 |
0.000 |
-24.305 |
|
| Traceless |
| | x | y | z |
| x |
-1.707 |
0.309 |
0.000 |
| y |
0.309 |
-1.029 |
0.000 |
| z |
0.000 |
0.000 |
2.736 |
|
| Polar |
| 3z2-r2 | 5.471 |
| x2-y2 | -0.452 |
| xy | 0.309 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.839 |
-0.580 |
0.000 |
| y |
-0.580 |
4.455 |
0.000 |
| z |
0.000 |
0.000 |
1.460 |
<r2> (average value of r
2) Å
2
| <r2> |
89.145 |
| (<r2>)1/2 |
9.442 |