Vibrational Frequencies calculated at HSEh1PBE/3-21G*
| 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 |
3621 |
3475 |
21.97 |
|
|
|
| 2 |
A |
1320 |
1267 |
0.05 |
|
|
|
| 3 |
A |
776 |
745 |
18.75 |
|
|
|
| 4 |
A |
668 |
642 |
169.83 |
|
|
|
| 5 |
A |
549 |
527 |
3.48 |
|
|
|
| 6 |
B |
3620 |
3475 |
182.55 |
|
|
|
| 7 |
B |
2342 |
2248 |
437.65 |
|
|
|
| 8 |
B |
785 |
754 |
576.89 |
|
|
|
| 9 |
B |
560 |
538 |
97.58 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7120.8 cm
-1
Scaled (by 0.9599) Zero Point Vibrational Energy (zpe) 6835.2 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 HSEh1PBE/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.789 |
|
|
|
| 2 |
N |
-0.726 |
|
|
|
| 3 |
N |
-0.726 |
|
|
|
| 4 |
H |
0.332 |
|
|
|
| 5 |
H |
0.332 |
|
|
|
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 |
2.279 |
2.279 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.537 |
4.638 |
0.000 |
| y |
4.638 |
-14.292 |
0.000 |
| z |
0.000 |
0.000 |
-17.167 |
|
| Traceless |
| | x | y | z |
| x |
-0.807 |
4.638 |
0.000 |
| y |
4.638 |
2.559 |
0.000 |
| z |
0.000 |
0.000 |
-1.753 |
|
| Polar |
| 3z2-r2 | -3.505 |
| x2-y2 | -2.244 |
| xy | 4.638 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.257 |
0.345 |
0.000 |
| y |
0.345 |
5.544 |
0.000 |
| z |
0.000 |
0.000 |
1.204 |
<r2> (average value of r
2) Å
2
| <r2> |
38.856 |
| (<r2>)1/2 |
6.233 |