Jump to
S1C2
Energy calculated at HSEh1PBE/6-31G*
| hartrees |
Energy at 0K | -168.400713 |
Energy at 298.15K | |
HF Energy | -168.400713 |
Nuclear repulsion energy | 60.493088 |
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/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 |
Σ |
3564 |
3389 |
246.69 |
25.63 |
0.23 |
0.38 |
2 |
Σ |
2407 |
2289 |
326.93 |
23.08 |
0.18 |
0.31 |
3 |
Σ |
1351 |
1284 |
112.26 |
18.51 |
0.28 |
0.43 |
4 |
Π |
585 |
556 |
0.09 |
0.90 |
0.75 |
0.86 |
4 |
Π |
585 |
556 |
0.09 |
0.90 |
0.75 |
0.86 |
5 |
Π |
258 |
246 |
92.87 |
2.34 |
0.75 |
0.86 |
5 |
Π |
258 |
246 |
92.87 |
2.34 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4503.2 cm
-1
Scaled (by 0.951) Zero Point Vibrational Energy (zpe) 4282.5 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/6-31G*
Point Group is C∞v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.000 |
0.000 |
1.181 |
N2 |
0.000 |
0.000 |
-0.018 |
C3 |
0.000 |
0.000 |
-1.180 |
H4 |
0.000 |
0.000 |
-2.243 |
Atom - Atom Distances (Å)
|
O1 |
N2 |
C3 |
H4 |
O1 | | 1.1994 | 2.3606 | 3.4242 |
N2 | 1.1994 | | 1.1612 | 2.2248 | C3 | 2.3606 | 1.1612 | | 1.0636 | H4 | 3.4242 | 2.2248 | 1.0636 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
N2 |
C3 |
180.000 |
|
N2 |
C3 |
H4 |
180.000 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.472 |
|
|
|
2 |
N |
0.196 |
|
|
|
3 |
C |
-0.018 |
|
|
|
4 |
H |
0.295 |
|
|
|
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 |
-3.140 |
3.140 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-16.429 |
0.000 |
0.000 |
y |
0.000 |
-16.429 |
0.000 |
z |
0.000 |
0.000 |
-13.433 |
|
Traceless |
| x | y | z |
x |
-1.498 |
0.000 |
0.000 |
y |
0.000 |
-1.498 |
0.000 |
z |
0.000 |
0.000 |
2.996 |
|
Polar |
3z2-r2 | 5.992 |
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 |
1.344 |
0.000 |
0.000 |
y |
0.000 |
1.344 |
0.000 |
z |
0.000 |
0.000 |
5.406 |
<r2> (average value of r
2) Å
2
<r2> |
34.179 |
(<r2>)1/2 |
5.846 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-31G*
| hartrees |
Energy at 0K | -168.400715 |
Energy at 298.15K | -168.401298 |
HF Energy | -168.400715 |
Nuclear repulsion energy | 60.495521 |
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/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' |
3564 |
3389 |
246.57 |
|
|
|
2 |
A' |
2407 |
2289 |
327.28 |
|
|
|
3 |
A' |
1351 |
1285 |
112.15 |
|
|
|
4 |
A' |
585 |
556 |
0.10 |
|
|
|
5 |
A' |
260 |
247 |
92.89 |
|
|
|
6 |
A" |
556 |
529 |
13.08 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4361.1 cm
-1
Scaled (by 0.951) Zero Point Vibrational Energy (zpe) 4147.4 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/6-31G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
-0.003 |
-1.181 |
0.000 |
N2 |
0.000 |
0.018 |
0.000 |
C3 |
0.004 |
1.180 |
0.000 |
H4 |
0.006 |
2.243 |
0.000 |
Atom - Atom Distances (Å)
|
O1 |
N2 |
C3 |
H4 |
O1 | | 1.1993 | 2.3605 | 3.4242 |
N2 | 1.1993 | | 1.1612 | 2.2250 | C3 | 2.3605 | 1.1612 | | 1.0637 | H4 | 3.4242 | 2.2250 | 1.0637 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
N2 |
C3 |
179.990 |
|
N2 |
C3 |
H4 |
179.974 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.472 |
|
|
|
2 |
N |
0.196 |
|
|
|
3 |
C |
-0.019 |
|
|
|
4 |
H |
0.295 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.009 |
3.139 |
0.000 |
3.139 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-16.429 |
0.008 |
0.000 |
y |
0.008 |
-13.433 |
0.000 |
z |
0.000 |
0.000 |
-16.429 |
|
Traceless |
| x | y | z |
x |
-1.498 |
0.008 |
0.000 |
y |
0.008 |
2.996 |
0.000 |
z |
0.000 |
0.000 |
-1.498 |
|
Polar |
3z2-r2 | -2.996 |
x2-y2 | -2.996 |
xy | 0.008 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.344 |
0.012 |
0.000 |
y |
0.012 |
5.407 |
0.000 |
z |
0.000 |
0.000 |
1.344 |
<r2> (average value of r
2) Å
2
<r2> |
34.178 |
(<r2>)1/2 |
5.846 |