Vibrational Frequencies calculated at LSDA/6-311G**
| 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 |
3593 |
3549 |
62.62 |
|
|
|
| 2 |
A |
3310 |
3269 |
0.25 |
|
|
|
| 3 |
A |
1598 |
1579 |
148.83 |
|
|
|
| 4 |
A |
1505 |
1487 |
109.67 |
|
|
|
| 5 |
A |
1201 |
1186 |
89.18 |
|
|
|
| 6 |
A |
1101 |
1087 |
28.76 |
|
|
|
| 7 |
A |
741 |
732 |
5.65 |
|
|
|
| 8 |
A |
609 |
602 |
0.81 |
|
|
|
| 9 |
A |
361 |
356 |
203.06 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7009.4 cm
-1
Scaled (by 0.9877) Zero Point Vibrational Energy (zpe) 6923.1 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/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.266 |
|
|
|
| 2 |
N |
0.081 |
|
|
|
| 3 |
N |
-0.288 |
|
|
|
| 4 |
H |
0.216 |
|
|
|
| 5 |
H |
0.256 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
3.615 |
0.728 |
0.001 |
3.687 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.302 |
0.201 |
0.004 |
| y |
0.201 |
-16.869 |
-0.003 |
| z |
0.004 |
-0.003 |
-17.528 |
|
| Traceless |
| | x | y | z |
| x |
1.897 |
0.201 |
0.004 |
| y |
0.201 |
-0.454 |
-0.003 |
| z |
0.004 |
-0.003 |
-1.443 |
|
| Polar |
| 3z2-r2 | -2.886 |
| x2-y2 | 1.567 |
| xy | 0.201 |
| xz | 0.004 |
| yz | -0.003 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.669 |
0.120 |
0.000 |
| y |
0.120 |
2.943 |
-0.000 |
| z |
0.000 |
-0.000 |
1.444 |
<r2> (average value of r
2) Å
2
| <r2> |
35.835 |
| (<r2>)1/2 |
5.986 |