Jump to
S1C2
S1C3
Energy calculated at LSDA/TZVP
| | hartrees |
| Energy at 0K | -99.783420 |
| Energy at 298.15K | -99.782542 |
| HF Energy | -99.783420 |
| Nuclear repulsion energy | 27.723670 |
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/TZVP
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
0.000 |
0.000 |
-2.056 |
| C2 |
0.000 |
0.000 |
-0.152 |
| N3 |
0.000 |
0.000 |
1.012 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 1.9041 | 3.0678 |
C2 | 1.9041 | | 1.1637 | N3 | 3.0678 | 1.1637 | |
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/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.468 |
|
|
|
| 2 |
C |
-0.374 |
|
|
|
| 3 |
N |
-0.094 |
|
|
|
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 |
-8.971 |
8.971 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.405 |
0.000 |
0.000 |
| y |
0.000 |
-14.405 |
0.000 |
| z |
0.000 |
0.000 |
0.655 |
|
| Traceless |
| | x | y | z |
| x |
-7.530 |
0.000 |
0.000 |
| y |
0.000 |
-7.530 |
0.000 |
| z |
0.000 |
0.000 |
15.059 |
|
| Polar |
| 3z2-r2 | 30.119 |
| 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 |
2.322 |
0.000 |
-0.001 |
| y |
0.000 |
2.322 |
0.000 |
| z |
-0.001 |
0.000 |
4.629 |
<r2> (average value of r
2) Å
2
| <r2> |
25.848 |
| (<r2>)1/2 |
5.084 |
Jump to
S1C1
S1C3
Energy calculated at LSDA/TZVP
| | hartrees |
| Energy at 0K | -99.783009 |
| Energy at 298.15K | -99.782309 |
| HF Energy | -99.783009 |
| Nuclear repulsion energy | 29.494085 |
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/TZVP
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
1.362 |
-0.675 |
0.000 |
| C2 |
-0.681 |
-0.359 |
0.000 |
| N3 |
0.000 |
0.597 |
0.000 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 2.0677 | 1.8643 |
C2 | 2.0677 | | 1.1743 | N3 | 1.8643 | 1.1743 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Li1 |
C2 |
N3 |
63.342 |
|
Li1 |
N3 |
C2 |
82.399 |
| C2 |
Li1 |
N3 |
34.259 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.535 |
|
|
|
| 2 |
C |
-0.247 |
|
|
|
| 3 |
N |
-0.288 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
6.131 |
-2.710 |
0.000 |
6.703 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-7.003 |
-6.094 |
0.000 |
| y |
-6.094 |
-15.103 |
0.000 |
| z |
0.000 |
0.000 |
-14.582 |
|
| Traceless |
| | x | y | z |
| x |
7.839 |
-6.094 |
0.000 |
| y |
-6.094 |
-4.310 |
0.000 |
| z |
0.000 |
0.000 |
-3.529 |
|
| Polar |
| 3z2-r2 | -7.058 |
| x2-y2 | 8.100 |
| xy | -6.094 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.848 |
0.167 |
0.000 |
| y |
0.167 |
3.521 |
0.000 |
| z |
0.000 |
0.000 |
2.620 |
<r2> (average value of r
2) Å
2
| <r2> |
20.630 |
| (<r2>)1/2 |
4.542 |
Jump to
S1C1
S1C2
Energy calculated at LSDA/TZVP
| | hartrees |
| Energy at 0K | -99.784962 |
| Energy at 298.15K | -99.783934 |
| HF Energy | -99.784962 |
| Nuclear repulsion energy | 28.427554 |
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/TZVP
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
0.000 |
0.000 |
1.880 |
| C2 |
0.000 |
0.000 |
-1.066 |
| N3 |
0.000 |
0.000 |
0.108 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 2.9460 | 1.7713 |
C2 | 2.9460 | | 1.1747 | N3 | 1.7713 | 1.1747 | |
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/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.675 |
|
|
|
| 2 |
C |
-0.274 |
|
|
|
| 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 |
| |
0.000 |
0.000 |
8.935 |
8.935 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.440 |
0.000 |
0.000 |
| y |
0.000 |
-14.440 |
0.000 |
| z |
0.000 |
0.000 |
-2.727 |
|
| Traceless |
| | x | y | z |
| x |
-5.857 |
0.000 |
0.000 |
| y |
0.000 |
-5.857 |
0.000 |
| z |
0.000 |
0.000 |
11.713 |
|
| Polar |
| 3z2-r2 | 23.427 |
| 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 |
2.366 |
0.000 |
0.000 |
| y |
0.000 |
2.366 |
-0.000 |
| z |
0.000 |
-0.000 |
4.831 |
<r2> (average value of r
2) Å
2
| <r2> |
24.084 |
| (<r2>)1/2 |
4.908 |