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 |
A1 |
3133 |
2980 |
153.77 |
|
|
|
| 2 |
A1 |
1641 |
1560 |
0.56 |
|
|
|
| 3 |
A1 |
1059 |
1007 |
106.62 |
|
|
|
| 4 |
E |
3104 |
2952 |
53.00 |
|
|
|
| 4 |
E |
3104 |
2952 |
53.01 |
|
|
|
| 5 |
E |
1692 |
1610 |
2.89 |
|
|
|
| 5 |
E |
1692 |
1610 |
2.89 |
|
|
|
| 6 |
E |
1223 |
1163 |
39.47 |
|
|
|
| 6 |
E |
1223 |
1163 |
39.47 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8935.4 cm
-1
Scaled (by 0.951) Zero Point Vibrational Energy (zpe) 8497.6 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 |
N |
-0.413 |
|
|
|
| 2 |
O |
-0.607 |
|
|
|
| 3 |
H |
0.340 |
|
|
|
| 4 |
H |
0.340 |
|
|
|
| 5 |
H |
0.340 |
|
|
|
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 |
-5.084 |
5.084 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.330 |
0.000 |
0.000 |
| y |
0.000 |
-11.330 |
0.000 |
| z |
0.000 |
0.000 |
-12.241 |
|
| Traceless |
| | x | y | z |
| x |
0.455 |
0.000 |
0.000 |
| y |
0.000 |
0.455 |
0.000 |
| z |
0.000 |
0.000 |
-0.911 |
|
| Polar |
| 3z2-r2 | -1.822 |
| x2-y2 | 0.000 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.735 |
0.000 |
0.000 |
| y |
0.000 |
1.735 |
0.000 |
| z |
0.000 |
0.000 |
2.885 |
<r2> (average value of r
2) Å
2
| <r2> |
19.823 |
| (<r2>)1/2 |
4.452 |