Vibrational Frequencies calculated at HSEh1PBE/cc-pVTZ
| 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 |
3738 |
3592 |
63.73 |
|
|
|
| 2 |
A |
3496 |
3360 |
8.76 |
|
|
|
| 3 |
A |
1643 |
1579 |
128.88 |
|
|
|
| 4 |
A |
1587 |
1525 |
140.72 |
|
|
|
| 5 |
A |
1240 |
1192 |
123.18 |
|
|
|
| 6 |
A |
1132 |
1088 |
63.95 |
|
|
|
| 7 |
A |
734 |
705 |
3.05 |
|
|
|
| 8 |
A |
636 |
611 |
1.02 |
|
|
|
| 9 |
A |
201 |
194 |
192.86 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7203.6 cm
-1
Scaled (by 0.9611) Zero Point Vibrational Energy (zpe) 6923.3 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/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.282 |
|
|
|
| 2 |
N |
0.083 |
|
|
|
| 3 |
N |
-0.099 |
|
|
|
| 4 |
H |
0.135 |
|
|
|
| 5 |
H |
0.163 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
3.604 |
0.705 |
-0.008 |
3.672 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.264 |
0.324 |
-0.015 |
| y |
0.324 |
-16.625 |
-0.002 |
| z |
-0.015 |
-0.002 |
-17.419 |
|
| Traceless |
| | x | y | z |
| x |
1.757 |
0.324 |
-0.015 |
| y |
0.324 |
-0.283 |
-0.002 |
| z |
-0.015 |
-0.002 |
-1.474 |
|
| Polar |
| 3z2-r2 | -2.948 |
| x2-y2 | 1.361 |
| xy | 0.324 |
| xz | -0.015 |
| yz | -0.002 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.653 |
0.035 |
-0.000 |
| y |
0.035 |
2.911 |
-0.000 |
| z |
-0.000 |
-0.000 |
1.781 |
<r2> (average value of r
2) Å
2
| <r2> |
35.604 |
| (<r2>)1/2 |
5.967 |