Vibrational Frequencies calculated at M06-2X/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 |
3704 |
3551 |
80.58 |
|
|
|
| 2 |
A |
3472 |
3329 |
33.25 |
|
|
|
| 3 |
A |
1595 |
1529 |
63.27 |
|
|
|
| 4 |
A |
1418 |
1360 |
60.93 |
|
|
|
| 5 |
A |
1168 |
1120 |
107.80 |
|
|
|
| 6 |
A |
1034 |
991 |
90.50 |
|
|
|
| 7 |
A |
703 |
674 |
34.87 |
|
|
|
| 8 |
A |
587 |
563 |
2.08 |
|
|
|
| 9 |
A |
408 |
391 |
350.92 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7044.4 cm
-1
Scaled (by 0.9587) Zero Point Vibrational Energy (zpe) 6753.5 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 M06-2X/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.346 |
|
|
|
| 2 |
N |
0.186 |
|
|
|
| 3 |
N |
-0.535 |
|
|
|
| 4 |
H |
0.339 |
|
|
|
| 5 |
H |
0.356 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
3.607 |
0.788 |
-0.004 |
3.692 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.143 |
0.380 |
-0.006 |
| y |
0.380 |
-16.286 |
-0.001 |
| z |
-0.006 |
-0.001 |
-17.268 |
|
| Traceless |
| | x | y | z |
| x |
1.634 |
0.380 |
-0.006 |
| y |
0.380 |
-0.080 |
-0.001 |
| z |
-0.006 |
-0.001 |
-1.553 |
|
| Polar |
| 3z2-r2 | -3.107 |
| x2-y2 | 1.143 |
| xy | 0.380 |
| xz | -0.006 |
| yz | -0.001 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.926 |
-0.128 |
0.000 |
| y |
-0.128 |
1.989 |
0.000 |
| z |
0.000 |
0.000 |
0.745 |
<r2> (average value of r
2) Å
2
| <r2> |
37.116 |
| (<r2>)1/2 |
6.092 |