Jump to
S1C2
Energy calculated at LSDA/TZVP
| | hartrees |
| Energy at 0K | -167.764036 |
| Energy at 298.15K | -167.764260 |
| HF Energy | -167.764036 |
| Nuclear repulsion energy | 60.684398 |
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 LSDA/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 |
Σ |
3440 |
3400 |
280.97 |
|
|
|
| 2 |
Σ |
2346 |
2319 |
368.77 |
|
|
|
| 3 |
Σ |
1336 |
1320 |
93.60 |
|
|
|
| 4 |
Π |
556 |
549 |
1.12 |
|
|
|
| 4 |
Π |
556 |
549 |
1.12 |
|
|
|
| 5 |
Π |
151 |
150 |
97.61 |
|
|
|
| 5 |
Π |
151 |
150 |
97.61 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4267.9 cm
-1
Scaled (by 0.9884) Zero Point Vibrational Energy (zpe) 4218.4 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 LSDA/TZVP
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.000 |
1.175 |
| N2 |
0.000 |
0.000 |
-0.013 |
| C3 |
0.000 |
0.000 |
-1.177 |
| H4 |
0.000 |
0.000 |
-2.247 |
Atom - Atom Distances (Å)
| |
O1 |
N2 |
C3 |
H4 |
| O1 | | 1.1887 | 2.3526 | 3.4226 |
N2 | 1.1887 | | 1.1640 | 2.2339 | C3 | 2.3526 | 1.1640 | | 1.0699 | H4 | 3.4226 | 2.2339 | 1.0699 | |
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 LSDA/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.220 |
|
|
|
| 2 |
N |
0.210 |
|
|
|
| 3 |
C |
-0.209 |
|
|
|
| 4 |
H |
0.219 |
|
|
|
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 |
-2.873 |
2.873 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.923 |
0.000 |
0.000 |
| y |
0.000 |
-16.923 |
0.000 |
| z |
0.000 |
0.000 |
-14.281 |
|
| Traceless |
| | x | y | z |
| x |
-1.321 |
0.000 |
0.000 |
| y |
0.000 |
-1.321 |
0.000 |
| z |
0.000 |
0.000 |
2.642 |
|
| Polar |
| 3z2-r2 | 5.284 |
| 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 |
1.668 |
0.000 |
0.000 |
| y |
0.000 |
1.668 |
0.000 |
| z |
0.000 |
0.000 |
6.200 |
<r2> (average value of r
2) Å
2
| <r2> |
34.439 |
| (<r2>)1/2 |
5.868 |
Jump to
S1C1
Energy calculated at LSDA/TZVP
| | hartrees |
| Energy at 0K | -167.764036 |
| Energy at 298.15K | -167.764463 |
| HF Energy | -167.764036 |
| Nuclear repulsion energy | 60.685994 |
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 LSDA/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' |
3438 |
3398 |
281.15 |
|
|
|
| 2 |
A' |
2346 |
2319 |
369.02 |
|
|
|
| 3 |
A' |
1336 |
1321 |
93.44 |
|
|
|
| 4 |
A' |
556 |
550 |
1.16 |
|
|
|
| 5 |
A' |
157 |
155 |
97.63 |
|
|
|
| 6 |
A" |
556 |
549 |
1.31 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4194.5 cm
-1
Scaled (by 0.9884) Zero Point Vibrational Energy (zpe) 4145.9 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.
Geometric Data calculated at LSDA/TZVP
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
-0.024 |
-1.175 |
0.000 |
| N2 |
0.000 |
0.013 |
0.000 |
| C3 |
0.025 |
1.177 |
0.000 |
| H4 |
0.041 |
2.247 |
0.000 |
Atom - Atom Distances (Å)
| |
O1 |
N2 |
C3 |
H4 |
| O1 | | 1.1885 | 2.3525 | 3.4227 |
N2 | 1.1885 | | 1.1640 | 2.2342 | C3 | 2.3525 | 1.1640 | | 1.0702 | H4 | 3.4227 | 2.2342 | 1.0702 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
N2 |
C3 |
179.917 |
|
N2 |
C3 |
H4 |
179.601 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.220 |
|
|
|
| 2 |
N |
0.210 |
|
|
|
| 3 |
C |
-0.209 |
|
|
|
| 4 |
H |
0.219 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.050 |
2.872 |
0.000 |
2.872 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.923 |
0.033 |
0.000 |
| y |
0.033 |
-14.281 |
0.000 |
| z |
0.000 |
0.000 |
-16.924 |
|
| Traceless |
| | x | y | z |
| x |
-1.321 |
0.033 |
0.000 |
| y |
0.033 |
2.643 |
0.000 |
| z |
0.000 |
0.000 |
-1.322 |
|
| Polar |
| 3z2-r2 | -2.643 |
| x2-y2 | -2.642 |
| xy | 0.033 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.670 |
0.097 |
0.000 |
| y |
0.097 |
6.198 |
0.000 |
| z |
0.000 |
0.000 |
1.668 |
<r2> (average value of r
2) Å
2
| <r2> |
34.438 |
| (<r2>)1/2 |
5.868 |