Vibrational Frequencies calculated at HSEh1PBE/6-31G(2df,p)
| 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 |
3760 |
3601 |
63.21 |
|
|
|
| 2 |
A |
3518 |
3370 |
11.42 |
|
|
|
| 3 |
A |
1664 |
1594 |
128.58 |
|
|
|
| 4 |
A |
1591 |
1523 |
116.26 |
|
|
|
| 5 |
A |
1248 |
1196 |
113.81 |
|
|
|
| 6 |
A |
1136 |
1088 |
49.78 |
|
|
|
| 7 |
A |
738 |
707 |
3.02 |
|
|
|
| 8 |
A |
633 |
606 |
1.48 |
|
|
|
| 9 |
A |
104 |
99 |
198.48 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7195.7 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 6891.3 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(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.329 |
|
|
|
| 2 |
N |
0.127 |
|
|
|
| 3 |
N |
-0.363 |
|
|
|
| 4 |
H |
0.269 |
|
|
|
| 5 |
H |
0.297 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
3.505 |
0.756 |
0.004 |
3.586 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.767 |
0.301 |
0.006 |
| y |
0.301 |
-16.232 |
0.001 |
| z |
0.006 |
0.001 |
-17.178 |
|
| Traceless |
| | x | y | z |
| x |
1.938 |
0.301 |
0.006 |
| y |
0.301 |
-0.260 |
0.001 |
| z |
0.006 |
0.001 |
-1.678 |
|
| Polar |
| 3z2-r2 | -3.357 |
| x2-y2 | 1.465 |
| xy | 0.301 |
| xz | 0.006 |
| yz | 0.001 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.347 |
0.040 |
0.000 |
| y |
0.040 |
2.663 |
0.000 |
| z |
0.000 |
0.000 |
1.626 |
<r2> (average value of r
2) Å
2
| <r2> |
35.423 |
| (<r2>)1/2 |
5.952 |