Vibrational Frequencies calculated at PBEPBE/Def2TZVPP
| 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 |
3600 |
3556 |
43.81 |
|
|
|
| 2 |
A |
3341 |
3300 |
0.80 |
|
|
|
| 3 |
A |
1535 |
1516 |
43.37 |
|
|
|
| 4 |
A |
1513 |
1494 |
186.10 |
|
|
|
| 5 |
A |
1174 |
1160 |
91.86 |
|
|
|
| 6 |
A |
1035 |
1023 |
82.16 |
|
|
|
| 7 |
A |
712 |
704 |
1.99 |
|
|
|
| 8 |
A |
598 |
590 |
0.25 |
|
|
|
| 9 |
A |
210 |
208 |
177.42 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6858.5 cm
-1
Scaled (by 0.9879) Zero Point Vibrational Energy (zpe) 6775.5 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 PBEPBE/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.284 |
|
|
|
| 2 |
N |
0.054 |
|
|
|
| 3 |
N |
-0.104 |
|
|
|
| 4 |
H |
0.148 |
|
|
|
| 5 |
H |
0.186 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
3.561 |
0.745 |
-0.001 |
3.638 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.419 |
0.331 |
-0.001 |
| y |
0.331 |
-17.031 |
-0.000 |
| z |
-0.001 |
-0.000 |
-17.722 |
|
| Traceless |
| | x | y | z |
| x |
1.957 |
0.331 |
-0.001 |
| y |
0.331 |
-0.460 |
-0.000 |
| z |
-0.001 |
-0.000 |
-1.497 |
|
| Polar |
| 3z2-r2 | -2.993 |
| x2-y2 | 1.612 |
| xy | 0.331 |
| xz | -0.001 |
| yz | -0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.200 |
0.094 |
0.000 |
| y |
0.094 |
3.326 |
0.000 |
| z |
0.000 |
0.000 |
2.046 |
<r2> (average value of r
2) Å
2
| <r2> |
36.508 |
| (<r2>)1/2 |
6.042 |