Jump to
S1C2
S1C3
Energy calculated at LSDA/3-21G
| | hartrees |
| Energy at 0K | -99.185111 |
| Energy at 298.15K | -99.184304 |
| HF Energy | -99.185111 |
| Nuclear repulsion energy | 27.511600 |
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/3-21G
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
0.000 |
0.000 |
-2.054 |
| C2 |
0.000 |
0.000 |
-0.160 |
| N3 |
0.000 |
0.000 |
1.018 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 1.8935 | 3.0717 |
C2 | 1.8935 | | 1.1782 | N3 | 3.0717 | 1.1782 | |
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/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.472 |
|
|
|
| 2 |
C |
-0.058 |
|
|
|
| 3 |
N |
-0.414 |
|
|
|
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 |
-8.237 |
8.237 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.466 |
0.000 |
0.000 |
| y |
0.000 |
-14.466 |
0.000 |
| z |
0.000 |
0.000 |
0.542 |
|
| Traceless |
| | x | y | z |
| x |
-7.504 |
0.000 |
0.000 |
| y |
0.000 |
-7.504 |
0.000 |
| z |
0.000 |
0.000 |
15.008 |
|
| Polar |
| 3z2-r2 | 30.016 |
| 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 |
2.330 |
0.000 |
0.000 |
| y |
0.000 |
2.330 |
0.000 |
| z |
0.000 |
0.000 |
4.178 |
<r2> (average value of r
2) Å
2
| <r2> |
25.972 |
| (<r2>)1/2 |
5.096 |
Jump to
S1C1
S1C3
Energy calculated at LSDA/3-21G
| | hartrees |
| Energy at 0K | -99.162341 |
| Energy at 298.15K | |
| HF Energy | -99.162341 |
| Nuclear repulsion energy | 25.738287 |
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/3-21G
Geometric Data calculated at LSDA/3-21G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
1.461 |
-0.536 |
0.000 |
| C2 |
-0.730 |
-0.383 |
0.000 |
| N3 |
0.000 |
0.559 |
0.000 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 2.1967 | 1.8257 |
C2 | 2.1967 | | 1.1921 | N3 | 1.8257 | 1.1921 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Li1 |
C2 |
N3 |
56.203 |
|
Li1 |
N3 |
C2 |
90.936 |
| C2 |
Li1 |
N3 |
32.861 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.449 |
|
|
|
| 2 |
C |
0.036 |
|
|
|
| 3 |
N |
-0.484 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
8.169 |
-1.087 |
0.000 |
8.241 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-0.933 |
-0.503 |
0.000 |
| y |
-0.503 |
-16.343 |
0.000 |
| z |
0.000 |
0.000 |
-14.983 |
|
| Traceless |
| | x | y | z |
| x |
14.730 |
-0.503 |
0.000 |
| y |
-0.503 |
-8.385 |
0.000 |
| z |
0.000 |
0.000 |
-6.345 |
|
| Polar |
| 3z2-r2 | -12.690 |
| x2-y2 | 15.410 |
| xy | -0.503 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.330 |
0.000 |
0.000 |
| y |
0.000 |
2.330 |
0.000 |
| z |
0.000 |
0.000 |
4.178 |
<r2> (average value of r
2) Å
2
| <r2> |
26.444 |
| (<r2>)1/2 |
5.142 |
Jump to
S1C1
S1C2
Energy calculated at LSDA/3-21G
| | hartrees |
| Energy at 0K | -99.192523 |
| Energy at 298.15K | -99.191490 |
| HF Energy | -99.192523 |
| Nuclear repulsion energy | 28.303899 |
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/3-21G
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
0.000 |
0.000 |
1.861 |
| C2 |
0.000 |
0.000 |
-1.070 |
| N3 |
0.000 |
0.000 |
0.120 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 2.9317 | 1.7416 |
C2 | 2.9317 | | 1.1902 | N3 | 1.7416 | 1.1902 | |
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/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.472 |
|
|
|
| 2 |
C |
0.065 |
|
|
|
| 3 |
N |
-0.537 |
|
|
|
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 |
8.188 |
8.188 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.389 |
0.000 |
0.000 |
| y |
0.000 |
-14.389 |
0.000 |
| z |
0.000 |
0.000 |
-3.178 |
|
| Traceless |
| | x | y | z |
| x |
-5.605 |
0.000 |
0.000 |
| y |
0.000 |
-5.605 |
0.000 |
| z |
0.000 |
0.000 |
11.211 |
|
| Polar |
| 3z2-r2 | 22.422 |
| 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 |
2.225 |
0.000 |
0.000 |
| y |
0.000 |
2.225 |
0.000 |
| z |
0.000 |
0.000 |
4.590 |
<r2> (average value of r
2) Å
2
| <r2> |
24.022 |
| (<r2>)1/2 |
4.901 |