Vibrational Frequencies calculated at B3LYP/aug-cc-pVQZ
| 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 |
3596 |
3484 |
23.81 |
|
|
|
| 2 |
A |
1289 |
1249 |
0.00 |
|
|
|
| 3 |
A |
917 |
888 |
14.26 |
|
|
|
| 4 |
A |
716 |
693 |
89.76 |
|
|
|
| 5 |
A |
545 |
528 |
0.44 |
|
|
|
| 6 |
B |
3593 |
3481 |
149.27 |
|
|
|
| 7 |
B |
2217 |
2148 |
704.40 |
|
|
|
| 8 |
B |
915 |
887 |
444.82 |
|
|
|
| 9 |
B |
548 |
531 |
72.54 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7167.0 cm
-1
Scaled (by 0.9689) Zero Point Vibrational Energy (zpe) 6944.1 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 B3LYP/aug-cc-pVQZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.563 |
|
|
|
| 2 |
N |
-0.619 |
|
|
|
| 3 |
N |
-0.619 |
|
|
|
| 4 |
H |
0.338 |
|
|
|
| 5 |
H |
0.338 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
1.940 |
1.940 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.134 |
4.087 |
0.000 |
| y |
4.087 |
-16.447 |
0.000 |
| z |
0.000 |
0.000 |
-17.638 |
|
| Traceless |
| | x | y | z |
| x |
-0.091 |
4.087 |
0.000 |
| y |
4.087 |
0.939 |
0.000 |
| z |
0.000 |
0.000 |
-0.848 |
|
| Polar |
| 3z2-r2 | -1.695 |
| x2-y2 | -0.687 |
| xy | 4.087 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.178 |
0.245 |
0.000 |
| y |
0.245 |
6.881 |
0.000 |
| z |
0.000 |
0.000 |
3.151 |
<r2> (average value of r
2) Å
2
| <r2> |
38.912 |
| (<r2>)1/2 |
6.238 |