Jump to
S1C2
S1C3
Energy calculated at B1B95/6-311G**
| | hartrees |
| Energy at 0K | -100.356167 |
| Energy at 298.15K | -100.355233 |
| HF Energy | -100.356167 |
| Nuclear repulsion energy | 27.771565 |
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 B1B95/6-311G**
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
0.000 |
0.000 |
-2.058 |
| C2 |
0.000 |
0.000 |
-0.150 |
| N3 |
0.000 |
0.000 |
1.010 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 1.9088 | 3.0688 |
C2 | 1.9088 | | 1.1600 | N3 | 3.0688 | 1.1600 | |
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 B1B95/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.593 |
|
|
|
| 2 |
C |
-0.283 |
|
|
|
| 3 |
N |
-0.310 |
|
|
|
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 |
-8.944 |
8.944 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.148 |
0.000 |
0.000 |
| y |
0.000 |
-14.148 |
0.000 |
| z |
0.000 |
0.000 |
1.207 |
|
| Traceless |
| | x | y | z |
| x |
-7.678 |
0.000 |
0.000 |
| y |
0.000 |
-7.678 |
0.000 |
| z |
0.000 |
0.000 |
15.355 |
|
| Polar |
| 3z2-r2 | 30.710 |
| 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 |
2.300 |
0.000 |
0.000 |
| y |
0.000 |
2.300 |
0.000 |
| z |
0.000 |
0.000 |
4.188 |
<r2> (average value of r
2) Å
2
| <r2> |
25.631 |
| (<r2>)1/2 |
5.063 |
Jump to
S1C1
S1C3
Energy calculated at B1B95/6-311G**
| | hartrees |
| Energy at 0K | -100.361012 |
| Energy at 298.15K | -100.360274 |
| HF Energy | -100.361012 |
| Nuclear repulsion energy | 29.457777 |
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 B1B95/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
1.406 |
-0.617 |
0.000 |
| C2 |
-0.703 |
-0.364 |
0.000 |
| N3 |
0.000 |
0.576 |
0.000 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 2.1235 | 1.8433 |
C2 | 2.1235 | | 1.1732 | N3 | 1.8433 | 1.1732 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Li1 |
C2 |
N3 |
60.046 |
|
Li1 |
N3 |
C2 |
86.486 |
| C2 |
Li1 |
N3 |
33.468 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.488 |
|
|
|
| 2 |
C |
-0.114 |
|
|
|
| 3 |
N |
-0.373 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
6.389 |
-2.528 |
0.000 |
6.871 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-6.193 |
-5.935 |
0.000 |
| y |
-5.935 |
-14.940 |
0.000 |
| z |
0.000 |
0.000 |
-14.348 |
|
| Traceless |
| | x | y | z |
| x |
8.451 |
-5.935 |
0.000 |
| y |
-5.935 |
-4.670 |
0.000 |
| z |
0.000 |
0.000 |
-3.782 |
|
| Polar |
| 3z2-r2 | -7.563 |
| x2-y2 | 8.748 |
| xy | -5.935 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.318 |
0.344 |
0.000 |
| y |
0.344 |
3.271 |
0.000 |
| z |
0.000 |
0.000 |
2.586 |
<r2> (average value of r
2) Å
2
| <r2> |
20.533 |
| (<r2>)1/2 |
4.531 |
Jump to
S1C1
S1C2
Energy calculated at B1B95/6-311G**
| | hartrees |
| Energy at 0K | -100.361169 |
| Energy at 298.15K | -100.360078 |
| HF Energy | -100.361169 |
| Nuclear repulsion energy | 28.485376 |
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 B1B95/6-311G**
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
0.000 |
0.000 |
1.875 |
| C2 |
0.000 |
0.000 |
-1.064 |
| N3 |
0.000 |
0.000 |
0.109 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 2.9386 | 1.7658 |
C2 | 2.9386 | | 1.1728 | N3 | 1.7658 | 1.1728 | |
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 B1B95/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.595 |
|
|
|
| 2 |
C |
-0.135 |
|
|
|
| 3 |
N |
-0.460 |
|
|
|
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 |
8.747 |
8.747 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.126 |
0.000 |
0.000 |
| y |
0.000 |
-14.126 |
0.000 |
| z |
0.000 |
0.000 |
-2.334 |
|
| Traceless |
| | x | y | z |
| x |
-5.896 |
0.000 |
0.000 |
| y |
0.000 |
-5.896 |
0.000 |
| z |
0.000 |
0.000 |
11.792 |
|
| Polar |
| 3z2-r2 | 23.584 |
| 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 |
2.323 |
0.000 |
0.000 |
| y |
0.000 |
2.323 |
0.000 |
| z |
0.000 |
0.000 |
4.369 |
<r2> (average value of r
2) Å
2
| <r2> |
23.786 |
| (<r2>)1/2 |
4.877 |