Jump to
S1C2
S1C3
Energy calculated at B2PLYP/cc-pCVTZ
| | hartrees |
| Energy at 0K | -100.330426 |
| Energy at 298.15K | -100.329500 |
| HF Energy | -100.212734 |
| Nuclear repulsion energy | 27.649324 |
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 B2PLYP/cc-pCVTZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
0.000 |
0.000 |
-2.062 |
| C2 |
0.000 |
0.000 |
-0.153 |
| N3 |
0.000 |
0.000 |
1.014 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 1.9092 | 3.0760 |
C2 | 1.9092 | | 1.1668 | N3 | 3.0760 | 1.1668 | |
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 B2PLYP/cc-pCVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.462 |
|
|
|
| 2 |
C |
-0.250 |
|
|
|
| 3 |
N |
-0.212 |
|
|
|
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 |
-9.014 |
9.014 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.299 |
0.000 |
0.000 |
| y |
0.000 |
-14.299 |
0.000 |
| z |
0.000 |
0.000 |
1.022 |
|
| Traceless |
| | x | y | z |
| x |
-7.661 |
0.000 |
0.000 |
| y |
0.000 |
-7.661 |
0.000 |
| z |
0.000 |
0.000 |
15.321 |
|
| Polar |
| 3z2-r2 | 30.642 |
| 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 |
2.707 |
0.000 |
0.000 |
| y |
0.000 |
2.707 |
0.000 |
| z |
0.000 |
0.000 |
4.303 |
<r2> (average value of r
2) Å
2
| <r2> |
25.835 |
| (<r2>)1/2 |
5.083 |
Jump to
S1C1
S1C3
Energy calculated at B2PLYP/cc-pCVTZ
| | hartrees |
| Energy at 0K | -100.333812 |
| Energy at 298.15K | -100.333067 |
| HF Energy | -100.217788 |
| Nuclear repulsion energy | 29.343446 |
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 B2PLYP/cc-pCVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
1.414 |
-0.608 |
0.000 |
| C2 |
-0.707 |
-0.367 |
0.000 |
| N3 |
0.000 |
0.576 |
0.000 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 2.1353 | 1.8445 |
C2 | 2.1353 | | 1.1786 | N3 | 1.8445 | 1.1786 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Li1 |
C2 |
N3 |
59.610 |
|
Li1 |
N3 |
C2 |
86.944 |
| C2 |
Li1 |
N3 |
33.446 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/cc-pCVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.320 |
|
|
|
| 2 |
C |
-0.108 |
|
|
|
| 3 |
N |
-0.212 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
6.446 |
-2.435 |
0.000 |
6.890 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-6.264 |
-5.982 |
0.000 |
| y |
-5.982 |
-15.125 |
0.000 |
| z |
0.000 |
0.000 |
-14.482 |
|
| Traceless |
| | x | y | z |
| x |
8.539 |
-5.982 |
0.000 |
| y |
-5.982 |
-4.752 |
0.000 |
| z |
0.000 |
0.000 |
-3.788 |
|
| Polar |
| 3z2-r2 | -7.576 |
| x2-y2 | 8.861 |
| xy | -5.982 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.591 |
0.365 |
0.000 |
| y |
0.365 |
3.549 |
0.000 |
| z |
0.000 |
0.000 |
2.923 |
<r2> (average value of r
2) Å
2
| <r2> |
20.709 |
| (<r2>)1/2 |
4.551 |
Jump to
S1C1
S1C2
Energy calculated at B2PLYP/cc-pCVTZ
| | hartrees |
| Energy at 0K | -100.334515 |
| Energy at 298.15K | -100.333419 |
| HF Energy | -100.220576 |
| Nuclear repulsion energy | 28.424107 |
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 B2PLYP/cc-pCVTZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
0.000 |
0.000 |
1.874 |
| C2 |
0.000 |
0.000 |
-1.066 |
| N3 |
0.000 |
0.000 |
0.111 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 2.9403 | 1.7633 |
C2 | 2.9403 | | 1.1771 | N3 | 1.7633 | 1.1771 | |
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 B2PLYP/cc-pCVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.397 |
|
|
|
| 2 |
C |
-0.206 |
|
|
|
| 3 |
N |
-0.190 |
|
|
|
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 |
8.874 |
8.874 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.358 |
0.000 |
0.000 |
| y |
0.000 |
-14.358 |
0.000 |
| z |
0.000 |
0.000 |
-2.573 |
|
| Traceless |
| | x | y | z |
| x |
-5.893 |
0.000 |
0.000 |
| y |
0.000 |
-5.893 |
0.000 |
| z |
0.000 |
0.000 |
11.786 |
|
| Polar |
| 3z2-r2 | 23.571 |
| 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 |
2.805 |
0.000 |
0.000 |
| y |
0.000 |
2.805 |
0.000 |
| z |
0.000 |
0.000 |
4.469 |
<r2> (average value of r
2) Å
2
| <r2> |
23.958 |
| (<r2>)1/2 |
4.895 |