Jump to
S1C2
S1C3
Energy calculated at HF/cc-pVDZ
| | hartrees |
| Energy at 0K | -99.781727 |
| Energy at 298.15K | -99.780738 |
| HF Energy | -99.781727 |
| Nuclear repulsion energy | 27.775116 |
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 HF/cc-pVDZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
0.000 |
0.000 |
-2.097 |
| C2 |
0.000 |
0.000 |
-0.135 |
| N3 |
0.000 |
0.000 |
1.014 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 1.9618 | 3.1106 |
C2 | 1.9618 | | 1.1488 | N3 | 3.1106 | 1.1488 | |
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 HF/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.492 |
|
|
|
| 2 |
C |
-0.262 |
|
|
|
| 3 |
N |
-0.230 |
|
|
|
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 |
-9.441 |
9.441 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.267 |
0.000 |
0.000 |
| y |
0.000 |
-14.267 |
0.000 |
| z |
0.000 |
0.000 |
2.499 |
|
| Traceless |
| | x | y | z |
| x |
-8.383 |
0.000 |
0.000 |
| y |
0.000 |
-8.383 |
0.000 |
| z |
0.000 |
0.000 |
16.766 |
|
| Polar |
| 3z2-r2 | 33.533 |
| 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 |
2.160 |
0.000 |
0.000 |
| y |
0.000 |
2.160 |
0.000 |
| z |
0.000 |
0.000 |
3.744 |
<r2> (average value of r
2) Å
2
| <r2> |
25.914 |
| (<r2>)1/2 |
5.091 |
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S1C1
S1C3
Energy calculated at HF/cc-pVDZ
| | hartrees |
| Energy at 0K | -99.793058 |
| Energy at 298.15K | |
| HF Energy | -99.793058 |
| Nuclear repulsion energy | 28.507581 |
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 HF/cc-pVDZ
Geometric Data calculated at HF/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
1.076 |
1.551 |
0.000 |
| C2 |
-0.538 |
-0.914 |
0.000 |
| N3 |
0.000 |
0.119 |
0.000 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 2.9475 | 1.7918 |
C2 | 2.9475 | | 1.1652 | N3 | 1.7918 | 1.1652 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Li1 |
C2 |
N3 |
5.706 |
|
Li1 |
N3 |
C2 |
170.586 |
| C2 |
Li1 |
N3 |
3.707 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.595 |
|
|
|
| 2 |
C |
-0.165 |
|
|
|
| 3 |
N |
-0.430 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
5.075 |
7.247 |
0.000 |
8.848 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-9.602 |
6.154 |
0.000 |
| y |
6.154 |
-6.090 |
0.000 |
| z |
0.000 |
0.000 |
-14.169 |
|
| Traceless |
| | x | y | z |
| x |
0.527 |
6.154 |
0.000 |
| y |
6.154 |
5.795 |
0.000 |
| z |
0.000 |
0.000 |
-6.322 |
|
| Polar |
| 3z2-r2 | -12.645 |
| x2-y2 | -3.512 |
| xy | 6.154 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.160 |
0.000 |
0.000 |
| y |
0.000 |
2.160 |
0.000 |
| z |
0.000 |
0.000 |
3.744 |
<r2> (average value of r
2) Å
2
| <r2> |
23.769 |
| (<r2>)1/2 |
4.875 |
Jump to
S1C1
S1C2
Energy calculated at HF/cc-pVDZ
| | hartrees |
| Energy at 0K | -99.793101 |
| Energy at 298.15K | -99.791894 |
| HF Energy | -99.793101 |
| Nuclear repulsion energy | 28.488971 |
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 HF/cc-pVDZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
0.000 |
0.000 |
1.894 |
| C2 |
0.000 |
0.000 |
-1.065 |
| N3 |
0.000 |
0.000 |
0.101 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 2.9585 | 1.7932 |
C2 | 2.9585 | | 1.1653 | N3 | 1.7932 | 1.1653 | |
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 HF/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.598 |
|
|
|
| 2 |
C |
-0.167 |
|
|
|
| 3 |
N |
-0.431 |
|
|
|
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 |
8.876 |
8.876 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.164 |
0.000 |
0.000 |
| y |
0.000 |
-14.164 |
0.000 |
| z |
0.000 |
0.000 |
-1.436 |
|
| Traceless |
| | x | y | z |
| x |
-6.364 |
0.000 |
0.000 |
| y |
0.000 |
-6.364 |
0.000 |
| z |
0.000 |
0.000 |
12.728 |
|
| Polar |
| 3z2-r2 | 25.457 |
| 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 |
2.141 |
0.000 |
0.000 |
| y |
0.000 |
2.141 |
0.000 |
| z |
0.000 |
0.000 |
3.906 |
<r2> (average value of r
2) Å
2
| <r2> |
23.828 |
| (<r2>)1/2 |
4.881 |