Vibrational Frequencies calculated at wB97X-D/6-31G*
| 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 |
3764 |
3570 |
61.75 |
|
|
|
| 2 |
A |
3545 |
3362 |
16.68 |
|
|
|
| 3 |
A |
1674 |
1588 |
118.35 |
|
|
|
| 4 |
A |
1618 |
1534 |
135.60 |
|
|
|
| 5 |
A |
1259 |
1194 |
114.33 |
|
|
|
| 6 |
A |
1139 |
1080 |
62.18 |
|
|
|
| 7 |
A |
726 |
689 |
6.08 |
|
|
|
| 8 |
A |
638 |
605 |
1.78 |
|
|
|
| 9 |
A |
125 |
119 |
278.62 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7243.3 cm
-1
Scaled (by 0.9485) Zero Point Vibrational Energy (zpe) 6870.2 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 wB97X-D/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.364 |
|
|
|
| 2 |
N |
0.176 |
|
|
|
| 3 |
N |
-0.542 |
|
|
|
| 4 |
H |
0.354 |
|
|
|
| 5 |
H |
0.375 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
3.626 |
0.756 |
0.274 |
3.715 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.932 |
0.326 |
0.462 |
| y |
0.326 |
-16.210 |
0.069 |
| z |
0.462 |
0.069 |
-17.292 |
|
| Traceless |
| | x | y | z |
| x |
1.818 |
0.326 |
0.462 |
| y |
0.326 |
-0.098 |
0.069 |
| z |
0.462 |
0.069 |
-1.720 |
|
| Polar |
| 3z2-r2 | -3.440 |
| x2-y2 | 1.278 |
| xy | 0.326 |
| xz | 0.462 |
| yz | 0.069 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.171 |
-0.026 |
0.001 |
| y |
-0.026 |
2.380 |
0.004 |
| z |
0.001 |
0.004 |
1.268 |
<r2> (average value of r
2) Å
2
| <r2> |
35.686 |
| (<r2>)1/2 |
5.974 |