Jump to
S1C2
S1C3
Energy calculated at LSDA/6-311G*
| | hartrees |
| Energy at 0K | -99.774516 |
| Energy at 298.15K | -99.773568 |
| HF Energy | -99.774516 |
| Nuclear repulsion energy | 27.752392 |
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/6-311G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
0.000 |
0.000 |
-2.046 |
| C2 |
0.000 |
0.000 |
-0.155 |
| N3 |
0.000 |
0.000 |
1.010 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 1.8903 | 3.0554 |
C2 | 1.8903 | | 1.1651 | N3 | 3.0554 | 1.1651 | |
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/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.542 |
|
|
|
| 2 |
C |
-0.269 |
|
|
|
| 3 |
N |
-0.273 |
|
|
|
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 |
-8.702 |
8.702 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.324 |
0.000 |
0.000 |
| y |
0.000 |
-14.324 |
0.000 |
| z |
0.000 |
0.000 |
0.650 |
|
| Traceless |
| | x | y | z |
| x |
-7.487 |
0.000 |
0.000 |
| y |
0.000 |
-7.487 |
0.000 |
| z |
0.000 |
0.000 |
14.974 |
|
| Polar |
| 3z2-r2 | 29.948 |
| 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 |
2.435 |
0.000 |
0.000 |
| y |
0.000 |
2.435 |
0.000 |
| z |
0.000 |
0.000 |
4.328 |
<r2> (average value of r
2) Å
2
| <r2> |
25.665 |
| (<r2>)1/2 |
5.066 |
Jump to
S1C1
S1C3
Energy calculated at LSDA/6-311G*
| | hartrees |
| Energy at 0K | -99.778893 |
| Energy at 298.15K | -99.778190 |
| HF Energy | -99.778893 |
| Nuclear repulsion energy | 29.546306 |
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/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
1.373 |
-0.625 |
0.000 |
| C2 |
-0.687 |
-0.370 |
0.000 |
| N3 |
0.000 |
0.585 |
0.000 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 2.0760 | 1.8310 |
C2 | 2.0760 | | 1.1767 | N3 | 1.8310 | 1.1767 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Li1 |
C2 |
N3 |
61.357 |
|
Li1 |
N3 |
C2 |
84.311 |
| C2 |
Li1 |
N3 |
34.333 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.427 |
|
|
|
| 2 |
C |
-0.111 |
|
|
|
| 3 |
N |
-0.316 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
6.102 |
-2.408 |
0.000 |
6.560 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-6.733 |
-5.830 |
0.000 |
| y |
-5.830 |
-15.191 |
0.000 |
| z |
0.000 |
0.000 |
-14.543 |
|
| Traceless |
| | x | y | z |
| x |
8.134 |
-5.830 |
0.000 |
| y |
-5.830 |
-4.553 |
0.000 |
| z |
0.000 |
0.000 |
-3.581 |
|
| Polar |
| 3z2-r2 | -7.162 |
| x2-y2 | 8.458 |
| xy | -5.830 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.528 |
0.254 |
0.000 |
| y |
0.254 |
3.429 |
0.000 |
| z |
0.000 |
0.000 |
2.754 |
<r2> (average value of r
2) Å
2
| <r2> |
20.475 |
| (<r2>)1/2 |
4.525 |
Jump to
S1C1
S1C2
Energy calculated at LSDA/6-311G*
| | hartrees |
| Energy at 0K | -99.778280 |
| Energy at 298.15K | -99.777194 |
| HF Energy | -99.778280 |
| Nuclear repulsion energy | 28.491336 |
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/6-311G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
0.000 |
0.000 |
1.864 |
| C2 |
0.000 |
0.000 |
-1.064 |
| N3 |
0.000 |
0.000 |
0.113 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 2.9272 | 1.7506 |
C2 | 2.9272 | | 1.1766 | N3 | 1.7506 | 1.1766 | |
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/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.547 |
|
|
|
| 2 |
C |
-0.160 |
|
|
|
| 3 |
N |
-0.387 |
|
|
|
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 |
8.643 |
8.643 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.336 |
0.000 |
0.000 |
| y |
0.000 |
-14.336 |
0.000 |
| z |
0.000 |
0.000 |
-2.886 |
|
| Traceless |
| | x | y | z |
| x |
-5.725 |
0.000 |
0.000 |
| y |
0.000 |
-5.725 |
0.000 |
| z |
0.000 |
0.000 |
11.450 |
|
| Polar |
| 3z2-r2 | 22.900 |
| 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 |
2.486 |
0.000 |
0.000 |
| y |
0.000 |
2.486 |
0.000 |
| z |
0.000 |
0.000 |
4.562 |
<r2> (average value of r
2) Å
2
| <r2> |
23.866 |
| (<r2>)1/2 |
4.885 |