Jump to
S1C2
S1C3
Energy calculated at LSDA/STO-3G
| | hartrees |
| Energy at 0K | -98.416019 |
| Energy at 298.15K | -98.415047 |
| HF Energy | -98.416019 |
| Nuclear repulsion energy | 27.130173 |
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/STO-3G
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
0.000 |
0.000 |
-2.022 |
| C2 |
0.000 |
0.000 |
-0.188 |
| N3 |
0.000 |
0.000 |
1.027 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 1.8339 | 3.0490 |
C2 | 1.8339 | | 1.2151 | N3 | 3.0490 | 1.2151 | |
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/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.189 |
|
|
|
| 2 |
C |
0.006 |
|
|
|
| 3 |
N |
-0.195 |
|
|
|
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 |
-6.390 |
6.390 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.317 |
0.000 |
0.000 |
| y |
0.000 |
-13.317 |
0.000 |
| z |
0.000 |
0.000 |
-0.598 |
|
| Traceless |
| | x | y | z |
| x |
-6.359 |
0.000 |
0.000 |
| y |
0.000 |
-6.359 |
0.000 |
| z |
0.000 |
0.000 |
12.719 |
|
| Polar |
| 3z2-r2 | 25.437 |
| 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 |
1.722 |
0.000 |
0.000 |
| y |
0.000 |
1.722 |
0.000 |
| z |
0.000 |
0.000 |
4.194 |
<r2> (average value of r
2) Å
2
| <r2> |
25.530 |
| (<r2>)1/2 |
5.053 |
Jump to
S1C1
S1C3
Energy calculated at LSDA/STO-3G
| | hartrees |
| Energy at 0K | -98.425580 |
| Energy at 298.15K | -98.425088 |
| HF Energy | -98.425580 |
| Nuclear repulsion energy | 29.446892 |
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/STO-3G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
1.241 |
-0.662 |
0.000 |
| C2 |
-0.621 |
-0.414 |
0.000 |
| N3 |
0.000 |
0.638 |
0.000 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 1.8783 | 1.7977 |
C2 | 1.8783 | | 1.2216 | N3 | 1.7977 | 1.2216 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Li1 |
C2 |
N3 |
67.063 |
|
Li1 |
N3 |
C2 |
74.197 |
| C2 |
Li1 |
N3 |
38.740 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.162 |
|
|
|
| 2 |
C |
0.037 |
|
|
|
| 3 |
N |
-0.198 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
3.720 |
-1.578 |
0.000 |
4.041 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-7.510 |
-4.583 |
0.000 |
| y |
-4.583 |
-14.797 |
0.000 |
| z |
0.000 |
0.000 |
-13.889 |
|
| Traceless |
| | x | y | z |
| x |
6.833 |
-4.583 |
0.000 |
| y |
-4.583 |
-4.097 |
0.000 |
| z |
0.000 |
0.000 |
-2.736 |
|
| Polar |
| 3z2-r2 | -5.471 |
| x2-y2 | 7.287 |
| xy | -4.583 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.870 |
-0.490 |
0.000 |
| y |
-0.490 |
2.139 |
0.000 |
| z |
0.000 |
0.000 |
1.782 |
<r2> (average value of r
2) Å
2
| <r2> |
19.664 |
| (<r2>)1/2 |
4.434 |
Jump to
S1C1
S1C2
Energy calculated at LSDA/STO-3G
| | hartrees |
| Energy at 0K | -98.413159 |
| Energy at 298.15K | -98.411939 |
| HF Energy | -98.413159 |
| Nuclear repulsion energy | 27.954534 |
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/STO-3G
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
0.000 |
0.000 |
1.822 |
| C2 |
0.000 |
0.000 |
-1.084 |
| N3 |
0.000 |
0.000 |
0.148 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 2.9064 | 1.6744 |
C2 | 2.9064 | | 1.2320 | N3 | 1.6744 | 1.2320 | |
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/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.260 |
|
|
|
| 2 |
C |
-0.007 |
|
|
|
| 3 |
N |
-0.253 |
|
|
|
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 |
5.806 |
5.806 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.188 |
0.000 |
0.000 |
| y |
0.000 |
-13.188 |
0.000 |
| z |
0.000 |
0.000 |
-4.039 |
|
| Traceless |
| | x | y | z |
| x |
-4.574 |
0.000 |
0.000 |
| y |
0.000 |
-4.574 |
0.000 |
| z |
0.000 |
0.000 |
9.149 |
|
| Polar |
| 3z2-r2 | 18.297 |
| 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 |
1.585 |
0.000 |
0.000 |
| y |
0.000 |
1.585 |
0.000 |
| z |
0.000 |
0.000 |
4.898 |
<r2> (average value of r
2) Å
2
| <r2> |
23.499 |
| (<r2>)1/2 |
4.848 |