Vibrational Frequencies calculated at B1B95/3-21G
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A' |
1549 |
1482 |
166.63 |
|
|
|
| 2 |
A' |
1164 |
1113 |
211.94 |
|
|
|
| 3 |
A' |
1085 |
1038 |
6.28 |
|
|
|
| 4 |
A' |
807 |
772 |
107.30 |
|
|
|
| 5 |
A' |
619 |
592 |
0.18 |
|
|
|
| 6 |
A' |
453 |
433 |
3.42 |
|
|
|
| 7 |
A' |
297 |
284 |
0.73 |
|
|
|
| 8 |
A" |
635 |
608 |
10.54 |
|
|
|
| 9 |
A" |
143 |
137 |
0.09 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3375.8 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 3229.7 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 B1B95/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
0.551 |
|
|
|
| 2 |
O |
-0.024 |
|
|
|
| 3 |
O |
-0.226 |
|
|
|
| 4 |
O |
-0.230 |
|
|
|
| 5 |
F |
-0.071 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.010 |
0.222 |
0.000 |
0.223 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-27.146 |
0.525 |
0.000 |
| y |
0.525 |
-26.760 |
0.000 |
| z |
0.000 |
0.000 |
-24.181 |
|
| Traceless |
| | x | y | z |
| x |
-1.675 |
0.525 |
0.000 |
| y |
0.525 |
-1.096 |
0.000 |
| z |
0.000 |
0.000 |
2.772 |
|
| Polar |
| 3z2-r2 | 5.543 |
| x2-y2 | -0.386 |
| xy | 0.525 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.591 |
-0.685 |
0.000 |
| y |
-0.685 |
4.383 |
0.000 |
| z |
0.000 |
0.000 |
0.666 |
<r2> (average value of r
2) Å
2
| <r2> |
94.547 |
| (<r2>)1/2 |
9.724 |