Vibrational Frequencies calculated at HSEh1PBE/6-311G**
| 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 |
3636 |
3492 |
30.17 |
|
|
|
| 2 |
A |
1307 |
1255 |
0.09 |
|
|
|
| 3 |
A |
912 |
876 |
9.71 |
|
|
|
| 4 |
A |
734 |
705 |
105.13 |
|
|
|
| 5 |
A |
542 |
521 |
0.28 |
|
|
|
| 6 |
B |
3634 |
3490 |
130.91 |
|
|
|
| 7 |
B |
2274 |
2184 |
619.78 |
|
|
|
| 8 |
B |
913 |
877 |
425.46 |
|
|
|
| 9 |
B |
545 |
523 |
85.77 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7247.8 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 6960.8 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/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.444 |
|
|
|
| 2 |
N |
-0.453 |
|
|
|
| 3 |
N |
-0.453 |
|
|
|
| 4 |
H |
0.231 |
|
|
|
| 5 |
H |
0.231 |
|
|
|
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 |
2.159 |
2.159 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.542 |
4.257 |
0.000 |
| y |
4.257 |
-16.225 |
0.000 |
| z |
0.000 |
0.000 |
-17.099 |
|
| Traceless |
| | x | y | z |
| x |
0.120 |
4.257 |
0.000 |
| y |
4.257 |
0.595 |
0.000 |
| z |
0.000 |
0.000 |
-0.716 |
|
| Polar |
| 3z2-r2 | -1.431 |
| x2-y2 | -0.317 |
| xy | 4.257 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.028 |
0.331 |
0.000 |
| y |
0.331 |
5.934 |
0.000 |
| z |
0.000 |
0.000 |
1.999 |
<r2> (average value of r
2) Å
2
| <r2> |
38.565 |
| (<r2>)1/2 |
6.210 |