Vibrational Frequencies calculated at HSEh1PBE/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 |
3652 |
3485 |
25.25 |
|
|
|
| 2 |
A |
1312 |
1252 |
0.11 |
|
|
|
| 3 |
A |
919 |
877 |
11.21 |
|
|
|
| 4 |
A |
742 |
708 |
108.21 |
|
|
|
| 5 |
A |
530 |
506 |
0.05 |
|
|
|
| 6 |
B |
3651 |
3484 |
114.46 |
|
|
|
| 7 |
B |
2281 |
2177 |
571.69 |
|
|
|
| 8 |
B |
918 |
876 |
441.71 |
|
|
|
| 9 |
B |
531 |
507 |
79.08 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7267.8 cm
-1
Scaled (by 0.9543) Zero Point Vibrational Energy (zpe) 6935.7 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/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.638 |
|
|
|
| 2 |
N |
-0.617 |
|
|
|
| 3 |
N |
-0.617 |
|
|
|
| 4 |
H |
0.298 |
|
|
|
| 5 |
H |
0.298 |
|
|
|
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 |
2.193 |
2.193 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.402 |
4.286 |
0.000 |
| y |
4.286 |
-15.969 |
0.000 |
| z |
0.000 |
0.000 |
-16.971 |
|
| Traceless |
| | x | y | z |
| x |
0.068 |
4.286 |
0.000 |
| y |
4.286 |
0.718 |
0.000 |
| z |
0.000 |
0.000 |
-0.786 |
|
| Polar |
| 3z2-r2 | -1.571 |
| x2-y2 | -0.433 |
| xy | 4.286 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.824 |
0.389 |
0.000 |
| y |
0.389 |
5.876 |
0.000 |
| z |
0.000 |
0.000 |
1.794 |
<r2> (average value of r
2) Å
2
| <r2> |
38.688 |
| (<r2>)1/2 |
6.220 |