Jump to
S1C2
Energy calculated at HSEh1PBE/TZVP
| | hartrees |
| Energy at 0K | -131.012135 |
| Energy at 298.15K | |
| HF Energy | -131.012135 |
| Nuclear repulsion energy | 35.290247 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at HSEh1PBE/TZVP
| 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 |
3461 |
3323 |
0.38 |
|
|
|
| 2 |
A1 |
1692 |
1625 |
13.47 |
|
|
|
| 3 |
A1 |
1423 |
1366 |
7.08 |
|
|
|
| 4 |
B1 |
23i |
22i |
214.40 |
|
|
|
| 5 |
B2 |
3595 |
3451 |
4.13 |
|
|
|
| 6 |
B2 |
1289 |
1237 |
3.26 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5718.3 cm
-1
Scaled (by 0.9601) Zero Point Vibrational Energy (zpe) 5490.1 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.
Geometric Data calculated at HSEh1PBE/TZVP
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-0.536 |
| O2 |
0.000 |
0.000 |
0.730 |
| H3 |
0.000 |
0.877 |
-1.045 |
| H4 |
0.000 |
-0.877 |
-1.045 |
Atom - Atom Distances (Å)
| |
N1 |
O2 |
H3 |
H4 |
| N1 | | 1.2662 | 1.0138 | 1.0138 |
O2 | 1.2662 | | 1.9799 | 1.9799 | H3 | 1.0138 | 1.9799 | | 1.7534 | H4 | 1.0138 | 1.9799 | 1.7534 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O2 |
N1 |
H3 |
120.144 |
|
O2 |
N1 |
H4 |
120.144 |
| H3 |
N1 |
H4 |
119.711 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.211 |
|
|
|
| 2 |
O |
-0.243 |
|
|
|
| 3 |
H |
0.227 |
|
|
|
| 4 |
H |
0.227 |
|
|
|
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 |
-3.136 |
3.136 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.543 |
0.000 |
0.000 |
| y |
0.000 |
-9.989 |
0.000 |
| z |
0.000 |
0.000 |
-11.112 |
|
| Traceless |
| | x | y | z |
| x |
-1.993 |
0.000 |
0.000 |
| y |
0.000 |
1.839 |
0.000 |
| z |
0.000 |
0.000 |
0.154 |
|
| Polar |
| 3z2-r2 | 0.309 |
| x2-y2 | -2.554 |
| 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 |
1.227 |
0.000 |
0.000 |
| y |
0.000 |
1.644 |
0.000 |
| z |
0.000 |
0.000 |
3.011 |
<r2> (average value of r
2) Å
2
| <r2> |
17.002 |
| (<r2>)1/2 |
4.123 |
Jump to
S1C1
Energy calculated at HSEh1PBE/TZVP
| | hartrees |
| Energy at 0K | -131.012135 |
| Energy at 298.15K | -131.013952 |
| HF Energy | -131.012135 |
| Nuclear repulsion energy | 35.290256 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at HSEh1PBE/TZVP
| 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' |
3461 |
3323 |
0.38 |
|
|
|
| 2 |
A' |
1692 |
1625 |
13.46 |
|
|
|
| 3 |
A' |
1423 |
1366 |
7.08 |
|
|
|
| 4 |
A' |
21 |
20 |
214.31 |
|
|
|
| 5 |
A" |
3594 |
3451 |
4.12 |
|
|
|
| 6 |
A" |
1289 |
1237 |
3.26 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5740.2 cm
-1
Scaled (by 0.9601) Zero Point Vibrational Energy (zpe) 5511.1 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.
Geometric Data calculated at HSEh1PBE/TZVP
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.211 |
|
|
|
| 2 |
O |
-0.243 |
|
|
|
| 3 |
H |
0.227 |
|
|
|
| 4 |
H |
0.227 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.040 |
3.136 |
0.000 |
3.136 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.543 |
0.037 |
0.000 |
| y |
0.037 |
-11.112 |
0.000 |
| z |
0.000 |
0.000 |
-9.989 |
|
| Traceless |
| | x | y | z |
| x |
-1.992 |
0.037 |
0.000 |
| y |
0.037 |
0.154 |
0.000 |
| z |
0.000 |
0.000 |
1.838 |
|
| Polar |
| 3z2-r2 | 3.676 |
| x2-y2 | -1.431 |
| xy | 0.037 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.227 |
0.005 |
0.000 |
| y |
0.005 |
3.011 |
0.000 |
| z |
0.000 |
0.000 |
1.644 |
<r2> (average value of r
2) Å
2
| <r2> |
17.002 |
| (<r2>)1/2 |
4.123 |