Vibrational Frequencies calculated at LSDA/STO-3G
| 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' |
1768 |
1584 |
26.33 |
|
|
|
| 2 |
A' |
1357 |
1215 |
37.97 |
|
|
|
| 3 |
A' |
1300 |
1164 |
48.15 |
|
|
|
| 4 |
A' |
814 |
729 |
27.95 |
|
|
|
| 5 |
A' |
599 |
537 |
1.64 |
|
|
|
| 6 |
A' |
418 |
374 |
0.19 |
|
|
|
| 7 |
A' |
225 |
201 |
0.17 |
|
|
|
| 8 |
A" |
504 |
452 |
1.10 |
|
|
|
| 9 |
A" |
173 |
155 |
0.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3579.4 cm
-1
Scaled (by 0.8955) Zero Point Vibrational Energy (zpe) 3205.3 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 LSDA/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
0.109 |
|
|
|
| 2 |
O |
0.006 |
|
|
|
| 3 |
O |
-0.077 |
|
|
|
| 4 |
O |
-0.069 |
|
|
|
| 5 |
F |
0.031 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.002 |
-0.695 |
0.000 |
0.695 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.975 |
0.310 |
0.000 |
| y |
0.310 |
-22.762 |
0.000 |
| z |
0.000 |
0.000 |
-21.663 |
|
| Traceless |
| | x | y | z |
| x |
-1.762 |
0.310 |
0.000 |
| y |
0.310 |
0.057 |
0.000 |
| z |
0.000 |
0.000 |
1.705 |
|
| Polar |
| 3z2-r2 | 3.410 |
| x2-y2 | -1.213 |
| xy | 0.310 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.507 |
-0.423 |
0.000 |
| y |
-0.423 |
3.723 |
0.000 |
| z |
0.000 |
0.000 |
0.389 |
<r2> (average value of r
2) Å
2
| <r2> |
0.000 |
| (<r2>)1/2 |
0.000 |