Vibrational Frequencies calculated at B3LYPultrafine/aug-cc-pVTZ
| 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' |
1820 |
1761 |
422.66 |
|
|
|
| 2 |
A' |
1345 |
1302 |
217.28 |
|
|
|
| 3 |
A' |
1009 |
976 |
43.44 |
|
|
|
| 4 |
A' |
816 |
790 |
158.97 |
|
|
|
| 5 |
A' |
654 |
632 |
4.67 |
|
|
|
| 6 |
A' |
457 |
442 |
30.17 |
|
|
|
| 7 |
A' |
294 |
284 |
2.24 |
|
|
|
| 8 |
A" |
727 |
703 |
10.40 |
|
|
|
| 9 |
A" |
161 |
156 |
0.12 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3641.2 cm
-1
Scaled (by 0.9675) Zero Point Vibrational Energy (zpe) 3522.8 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 B3LYPultrafine/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
1.032 |
|
|
|
| 2 |
O |
-0.055 |
|
|
|
| 3 |
O |
-0.383 |
|
|
|
| 4 |
O |
-0.416 |
|
|
|
| 5 |
F |
-0.178 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.027 |
0.157 |
0.000 |
0.160 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-27.880 |
0.403 |
0.000 |
| y |
0.403 |
-27.757 |
0.000 |
| z |
0.000 |
0.000 |
-24.954 |
|
| Traceless |
| | x | y | z |
| x |
-1.525 |
0.403 |
0.000 |
| y |
0.403 |
-1.340 |
0.000 |
| z |
0.000 |
0.000 |
2.865 |
|
| Polar |
| 3z2-r2 | 5.729 |
| x2-y2 | -0.123 |
| xy | 0.403 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.870 |
-0.462 |
0.000 |
| y |
-0.462 |
5.839 |
0.000 |
| z |
0.000 |
0.000 |
2.569 |
<r2> (average value of r
2) Å
2
| <r2> |
91.807 |
| (<r2>)1/2 |
9.582 |