Vibrational Frequencies calculated at B97D3/aug-cc-pVTZ
| 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 |
3623 |
3567 |
41.29 |
|
|
|
| 2 |
A |
3362 |
3310 |
1.19 |
|
|
|
| 3 |
A |
1553 |
1529 |
10.93 |
|
|
|
| 4 |
A |
1519 |
1495 |
220.76 |
|
|
|
| 5 |
A |
1181 |
1163 |
92.77 |
|
|
|
| 6 |
A |
1021 |
1005 |
110.96 |
|
|
|
| 7 |
A |
709 |
698 |
1.86 |
|
|
|
| 8 |
A |
605 |
596 |
0.21 |
|
|
|
| 9 |
A |
201 |
198 |
180.29 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6885.9 cm
-1
Scaled (by 0.9847) Zero Point Vibrational Energy (zpe) 6780.6 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 B97D3/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.412 |
|
|
|
| 2 |
N |
0.053 |
|
|
|
| 3 |
N |
0.140 |
|
|
|
| 4 |
H |
0.095 |
|
|
|
| 5 |
H |
0.123 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
3.568 |
0.737 |
-0.001 |
3.643 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.488 |
0.423 |
-0.002 |
| y |
0.423 |
-17.142 |
-0.000 |
| z |
-0.002 |
-0.000 |
-17.824 |
|
| Traceless |
| | x | y | z |
| x |
1.994 |
0.423 |
-0.002 |
| y |
0.423 |
-0.486 |
-0.000 |
| z |
-0.002 |
-0.000 |
-1.509 |
|
| Polar |
| 3z2-r2 | -3.018 |
| x2-y2 | 1.653 |
| xy | 0.423 |
| xz | -0.002 |
| yz | -0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.686 |
0.084 |
0.000 |
| y |
0.084 |
3.905 |
-0.000 |
| z |
0.000 |
-0.000 |
2.726 |
<r2> (average value of r
2) Å
2
| <r2> |
36.491 |
| (<r2>)1/2 |
6.041 |