Jump to
S1C2
S1C3
Energy calculated at LSDA/6-31G**
| | hartrees |
| Energy at 0K | -99.741147 |
| Energy at 298.15K | -99.740186 |
| HF Energy | -99.741147 |
| Nuclear repulsion energy | 27.538177 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Geometric Data calculated at LSDA/6-31G**
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
0.000 |
0.000 |
-2.062 |
| C2 |
0.000 |
0.000 |
-0.156 |
| N3 |
0.000 |
0.000 |
1.018 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 1.9051 | 3.0792 |
C2 | 1.9051 | | 1.1741 | N3 | 3.0792 | 1.1741 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Li1 |
C2 |
N3 |
180.000 |
|
Li1 |
N3 |
C2 |
0.000 |
| C2 |
Li1 |
N3 |
0.000 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.434 |
|
|
|
| 2 |
C |
-0.028 |
|
|
|
| 3 |
N |
-0.407 |
|
|
|
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 |
-8.545 |
8.545 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.234 |
0.000 |
0.000 |
| y |
0.000 |
-14.234 |
0.000 |
| z |
0.000 |
0.000 |
1.141 |
|
| Traceless |
| | x | y | z |
| x |
-7.687 |
0.000 |
0.000 |
| y |
0.000 |
-7.687 |
0.000 |
| z |
0.000 |
0.000 |
15.375 |
|
| Polar |
| 3z2-r2 | 30.750 |
| 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 |
2.488 |
0.000 |
0.000 |
| y |
0.000 |
2.488 |
0.000 |
| z |
0.000 |
0.000 |
4.571 |
<r2> (average value of r
2) Å
2
| <r2> |
25.835 |
| (<r2>)1/2 |
5.083 |
Jump to
S1C1
S1C3
Energy calculated at LSDA/6-31G**
| | hartrees |
| Energy at 0K | -99.746863 |
| Energy at 298.15K | -99.746185 |
| HF Energy | -99.746863 |
| Nuclear repulsion energy | 29.276703 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Geometric Data calculated at LSDA/6-31G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
1.388 |
-0.633 |
0.000 |
| C2 |
-0.694 |
-0.372 |
0.000 |
| N3 |
0.000 |
0.590 |
0.000 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 2.0987 | 1.8504 |
C2 | 2.0987 | | 1.1865 | N3 | 1.8504 | 1.1865 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Li1 |
C2 |
N3 |
61.339 |
|
Li1 |
N3 |
C2 |
84.422 |
| C2 |
Li1 |
N3 |
34.239 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.326 |
|
|
|
| 2 |
C |
0.074 |
|
|
|
| 3 |
N |
-0.401 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
6.017 |
-2.470 |
0.000 |
6.504 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-6.412 |
-5.820 |
0.000 |
| y |
-5.820 |
-15.217 |
0.000 |
| z |
0.000 |
0.000 |
-14.719 |
|
| Traceless |
| | x | y | z |
| x |
8.557 |
-5.820 |
0.000 |
| y |
-5.820 |
-4.652 |
0.000 |
| z |
0.000 |
0.000 |
-3.905 |
|
| Polar |
| 3z2-r2 | -7.810 |
| x2-y2 | 8.806 |
| xy | -5.820 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.416 |
0.252 |
0.000 |
| y |
0.252 |
3.411 |
0.000 |
| z |
0.000 |
0.000 |
2.745 |
<r2> (average value of r
2) Å
2
| <r2> |
20.712 |
| (<r2>)1/2 |
4.551 |
Jump to
S1C1
S1C2
Energy calculated at LSDA/6-31G**
| | hartrees |
| Energy at 0K | -99.741357 |
| Energy at 298.15K | |
| HF Energy | -99.741357 |
| Nuclear repulsion energy | 28.239069 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Geometric Data calculated at LSDA/6-31G**
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
0.000 |
0.000 |
1.882 |
| C2 |
0.000 |
0.000 |
-1.073 |
| N3 |
0.000 |
0.000 |
0.113 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 2.9555 | 1.7692 |
C2 | 2.9555 | | 1.1863 | N3 | 1.7692 | 1.1863 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Li1 |
C2 |
N3 |
0.000 |
|
Li1 |
N3 |
C2 |
180.000 |
| C2 |
Li1 |
N3 |
0.000 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.530 |
|
|
|
| 2 |
C |
-0.110 |
|
|
|
| 3 |
N |
-0.420 |
|
|
|
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 |
8.422 |
8.422 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.208 |
0.000 |
0.000 |
| y |
0.000 |
-14.208 |
0.000 |
| z |
0.000 |
0.000 |
-2.044 |
|
| Traceless |
| | x | y | z |
| x |
-6.082 |
0.000 |
0.000 |
| y |
0.000 |
-6.082 |
0.000 |
| z |
0.000 |
0.000 |
12.164 |
|
| Polar |
| 3z2-r2 | 24.328 |
| 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 |
2.429 |
0.000 |
0.000 |
| y |
0.000 |
2.429 |
0.000 |
| z |
0.000 |
0.000 |
4.757 |
<r2> (average value of r
2) Å
2
| <r2> |
23.971 |
| (<r2>)1/2 |
4.896 |