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 |
3745 |
3562 |
60.00 |
|
|
|
| 2 |
A |
3513 |
3340 |
10.50 |
|
|
|
| 3 |
A |
1670 |
1589 |
125.22 |
|
|
|
| 4 |
A |
1614 |
1535 |
128.71 |
|
|
|
| 5 |
A |
1260 |
1198 |
115.38 |
|
|
|
| 6 |
A |
1145 |
1089 |
49.25 |
|
|
|
| 7 |
A |
743 |
707 |
5.18 |
|
|
|
| 8 |
A |
633 |
602 |
1.77 |
|
|
|
| 9 |
A |
68 |
65 |
261.14 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7195.4 cm
-1
Scaled (by 0.951) Zero Point Vibrational Energy (zpe) 6842.9 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 |
O |
-0.362 |
|
|
|
| 2 |
N |
0.171 |
|
|
|
| 3 |
N |
-0.532 |
|
|
|
| 4 |
H |
0.349 |
|
|
|
| 5 |
H |
0.373 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
3.619 |
0.753 |
0.129 |
3.699 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.910 |
0.311 |
0.219 |
| y |
0.311 |
-16.280 |
0.030 |
| z |
0.219 |
0.030 |
-17.315 |
|
| Traceless |
| | x | y | z |
| x |
1.888 |
0.311 |
0.219 |
| y |
0.311 |
-0.167 |
0.030 |
| z |
0.219 |
0.030 |
-1.720 |
|
| Polar |
| 3z2-r2 | -3.440 |
| x2-y2 | 1.370 |
| xy | 0.311 |
| xz | 0.219 |
| yz | 0.030 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.221 |
-0.003 |
0.002 |
| y |
-0.003 |
2.438 |
0.002 |
| z |
0.002 |
0.002 |
1.265 |
<r2> (average value of r
2) Å
2
| <r2> |
35.640 |
| (<r2>)1/2 |
5.970 |