Jump to
S1C2
S1C3
Energy calculated at B1B95/cc-pVTZ
| | hartrees |
| Energy at 0K | -100.365564 |
| Energy at 298.15K | -100.364641 |
| HF Energy | -100.365564 |
| Nuclear repulsion energy | 27.814954 |
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 B1B95/cc-pVTZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
0.000 |
0.000 |
-2.057 |
| C2 |
0.000 |
0.000 |
-0.149 |
| N3 |
0.000 |
0.000 |
1.009 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 1.9087 | 3.0662 |
C2 | 1.9087 | | 1.1576 | N3 | 3.0662 | 1.1576 | |
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 B1B95/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.403 |
|
|
|
| 2 |
C |
-0.269 |
|
|
|
| 3 |
N |
-0.134 |
|
|
|
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 |
-9.031 |
9.031 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.170 |
0.000 |
0.000 |
| y |
0.000 |
-14.170 |
0.000 |
| z |
0.000 |
0.000 |
1.209 |
|
| Traceless |
| | x | y | z |
| x |
-7.690 |
0.000 |
0.000 |
| y |
0.000 |
-7.690 |
0.000 |
| z |
0.000 |
0.000 |
15.379 |
|
| Polar |
| 3z2-r2 | 30.759 |
| 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 |
2.607 |
0.000 |
0.000 |
| y |
0.000 |
2.607 |
0.000 |
| z |
0.000 |
0.000 |
4.227 |
<r2> (average value of r
2) Å
2
| <r2> |
25.604 |
| (<r2>)1/2 |
5.060 |
Jump to
S1C1
S1C3
Energy calculated at B1B95/cc-pVTZ
| | hartrees |
| Energy at 0K | -100.370161 |
| Energy at 298.15K | -100.369412 |
| HF Energy | -100.370161 |
| Nuclear repulsion energy | 29.500955 |
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 B1B95/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
1.406 |
-0.616 |
0.000 |
| C2 |
-0.703 |
-0.362 |
0.000 |
| N3 |
0.000 |
0.574 |
0.000 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 2.1250 | 1.8425 |
C2 | 2.1250 | | 1.1706 | N3 | 1.8425 | 1.1706 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Li1 |
C2 |
N3 |
59.950 |
|
Li1 |
N3 |
C2 |
86.689 |
| C2 |
Li1 |
N3 |
33.362 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.288 |
|
|
|
| 2 |
C |
-0.139 |
|
|
|
| 3 |
N |
-0.149 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
6.410 |
-2.495 |
0.000 |
6.879 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-6.173 |
-5.968 |
0.000 |
| y |
-5.968 |
-14.875 |
0.000 |
| z |
0.000 |
0.000 |
-14.319 |
|
| Traceless |
| | x | y | z |
| x |
8.424 |
-5.968 |
0.000 |
| y |
-5.968 |
-4.629 |
0.000 |
| z |
0.000 |
0.000 |
-3.794 |
|
| Polar |
| 3z2-r2 | -7.589 |
| x2-y2 | 8.702 |
| xy | -5.968 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.547 |
0.374 |
0.000 |
| y |
0.374 |
3.514 |
0.000 |
| z |
0.000 |
0.000 |
2.887 |
<r2> (average value of r
2) Å
2
| <r2> |
20.496 |
| (<r2>)1/2 |
4.527 |
Jump to
S1C1
S1C2
Energy calculated at B1B95/cc-pVTZ
| | hartrees |
| Energy at 0K | -100.370575 |
| Energy at 298.15K | -100.369471 |
| HF Energy | -100.370575 |
| Nuclear repulsion energy | 28.553629 |
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 B1B95/cc-pVTZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
0.000 |
0.000 |
1.871 |
| C2 |
0.000 |
0.000 |
-1.062 |
| N3 |
0.000 |
0.000 |
0.108 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 2.9322 | 1.7624 |
C2 | 2.9322 | | 1.1698 | N3 | 1.7624 | 1.1698 | |
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 B1B95/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.360 |
|
|
|
| 2 |
C |
-0.304 |
|
|
|
| 3 |
N |
-0.056 |
|
|
|
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 |
8.833 |
8.833 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.208 |
0.000 |
0.000 |
| y |
0.000 |
-14.208 |
0.000 |
| z |
0.000 |
0.000 |
-2.388 |
|
| Traceless |
| | x | y | z |
| x |
-5.910 |
0.000 |
0.000 |
| y |
0.000 |
-5.910 |
0.000 |
| z |
0.000 |
0.000 |
11.820 |
|
| Polar |
| 3z2-r2 | 23.640 |
| 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 |
2.775 |
0.000 |
0.000 |
| y |
0.000 |
2.775 |
0.000 |
| z |
0.000 |
0.000 |
4.416 |
<r2> (average value of r
2) Å
2
| <r2> |
23.755 |
| (<r2>)1/2 |
4.874 |