Jump to
S1C2
S1C3
Energy calculated at LSDA/cc-pVTZ
| | hartrees |
| Energy at 0K | -99.786578 |
| Energy at 298.15K | -99.785637 |
| HF Energy | -99.786578 |
| Nuclear repulsion energy | 27.792295 |
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/cc-pVTZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
0.000 |
0.000 |
-2.045 |
| C2 |
0.000 |
0.000 |
-0.154 |
| N3 |
0.000 |
0.000 |
1.009 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 1.8905 | 3.0533 |
C2 | 1.8905 | | 1.1628 | N3 | 3.0533 | 1.1628 | |
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/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.316 |
|
|
|
| 2 |
C |
-0.217 |
|
|
|
| 3 |
N |
-0.099 |
|
|
|
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 |
-8.805 |
8.805 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.342 |
0.000 |
0.000 |
| y |
0.000 |
-14.342 |
0.000 |
| z |
0.000 |
0.000 |
0.650 |
|
| Traceless |
| | x | y | z |
| x |
-7.496 |
0.000 |
0.000 |
| y |
0.000 |
-7.496 |
0.000 |
| z |
0.000 |
0.000 |
14.992 |
|
| Polar |
| 3z2-r2 | 29.985 |
| 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 |
2.828 |
0.000 |
0.000 |
| y |
0.000 |
2.828 |
0.000 |
| z |
0.000 |
0.000 |
4.413 |
<r2> (average value of r
2) Å
2
| <r2> |
25.643 |
| (<r2>)1/2 |
5.064 |
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S1C1
S1C3
Energy calculated at LSDA/cc-pVTZ
| | hartrees |
| Energy at 0K | -99.790661 |
| Energy at 298.15K | -99.789961 |
| HF Energy | -99.790661 |
| Nuclear repulsion energy | 29.598551 |
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/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
1.368 |
-0.631 |
0.000 |
| C2 |
-0.684 |
-0.368 |
0.000 |
| N3 |
0.000 |
0.586 |
0.000 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 2.0696 | 1.8317 |
C2 | 2.0696 | | 1.1741 | N3 | 1.8317 | 1.1741 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Li1 |
C2 |
N3 |
61.665 |
|
Li1 |
N3 |
C2 |
83.986 |
| C2 |
Li1 |
N3 |
34.348 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.200 |
|
|
|
| 2 |
C |
-0.116 |
|
|
|
| 3 |
N |
-0.084 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
6.105 |
-2.410 |
0.000 |
6.563 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-6.773 |
-5.888 |
0.000 |
| y |
-5.888 |
-15.119 |
0.000 |
| z |
0.000 |
0.000 |
-14.499 |
|
| Traceless |
| | x | y | z |
| x |
8.036 |
-5.888 |
0.000 |
| y |
-5.888 |
-4.483 |
0.000 |
| z |
0.000 |
0.000 |
-3.553 |
|
| Polar |
| 3z2-r2 | -7.106 |
| x2-y2 | 8.346 |
| xy | -5.888 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.761 |
0.293 |
0.000 |
| y |
0.293 |
3.687 |
0.000 |
| z |
0.000 |
0.000 |
3.040 |
<r2> (average value of r
2) Å
2
| <r2> |
20.417 |
| (<r2>)1/2 |
4.519 |
Jump to
S1C1
S1C2
Energy calculated at LSDA/cc-pVTZ
| | hartrees |
| Energy at 0K | -99.790215 |
| Energy at 298.15K | -99.789106 |
| HF Energy | -99.790215 |
| Nuclear repulsion energy | 28.552305 |
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/cc-pVTZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
0.000 |
0.000 |
1.860 |
| C2 |
0.000 |
0.000 |
-1.061 |
| N3 |
0.000 |
0.000 |
0.113 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 2.9216 | 1.7477 |
C2 | 2.9216 | | 1.1739 | N3 | 1.7477 | 1.1739 | |
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/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.290 |
|
|
|
| 2 |
C |
-0.315 |
|
|
|
| 3 |
N |
0.025 |
|
|
|
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 |
8.745 |
8.745 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.408 |
0.000 |
0.000 |
| y |
0.000 |
-14.408 |
0.000 |
| z |
0.000 |
0.000 |
-2.945 |
|
| Traceless |
| | x | y | z |
| x |
-5.731 |
0.000 |
0.000 |
| y |
0.000 |
-5.731 |
0.000 |
| z |
0.000 |
0.000 |
11.462 |
|
| Polar |
| 3z2-r2 | 22.925 |
| 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 |
2.928 |
0.000 |
0.000 |
| y |
0.000 |
2.928 |
-0.000 |
| z |
0.000 |
-0.000 |
4.621 |
<r2> (average value of r
2) Å
2
| <r2> |
23.841 |
| (<r2>)1/2 |
4.883 |