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S1C2
S1C3
Energy calculated at PBE1PBE/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -100.274905 |
| Energy at 298.15K | -100.273988 |
| HF Energy | -100.274905 |
| Nuclear repulsion energy | 27.778760 |
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 PBE1PBE/aug-cc-pVTZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Σ |
2253 |
2166 |
7.82 |
|
|
|
| 2 |
Σ |
637 |
612 |
127.99 |
|
|
|
| 3 |
Π |
175 |
168 |
34.14 |
|
|
|
| 3 |
Π |
175 |
168 |
34.14 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1619.3 cm
-1
Scaled (by 0.9615) Zero Point Vibrational Energy (zpe) 1556.9 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at PBE1PBE/aug-cc-pVTZ
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 |
-0.149 |
| N3 |
0.000 |
0.000 |
1.010 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 1.9086 | 3.0683 |
C2 | 1.9086 | | 1.1596 | N3 | 3.0683 | 1.1596 | |
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 PBE1PBE/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.175 |
|
|
|
| 2 |
C |
0.206 |
|
|
|
| 3 |
N |
-0.380 |
|
|
|
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 |
-9.165 |
9.165 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.312 |
0.000 |
0.000 |
| y |
0.000 |
-14.312 |
0.000 |
| z |
0.000 |
0.000 |
0.939 |
|
| Traceless |
| | x | y | z |
| x |
-7.625 |
0.000 |
0.000 |
| y |
0.000 |
-7.625 |
0.000 |
| z |
0.000 |
0.000 |
15.251 |
|
| Polar |
| 3z2-r2 | 30.501 |
| 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 |
3.143 |
0.000 |
0.000 |
| y |
0.000 |
3.143 |
0.000 |
| z |
0.000 |
0.000 |
4.624 |
<r2> (average value of r
2) Å
2
| <r2> |
25.748 |
| (<r2>)1/2 |
5.074 |
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S1C1
S1C3
Energy calculated at PBE1PBE/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -100.278024 |
| Energy at 298.15K | -100.277275 |
| HF Energy | -100.278024 |
| Nuclear repulsion energy | 29.482567 |
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 PBE1PBE/aug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
1.411 |
-0.605 |
0.000 |
| C2 |
-0.705 |
-0.365 |
0.000 |
| N3 |
0.000 |
0.572 |
0.000 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 2.1295 | 1.8367 |
C2 | 2.1295 | | 1.1723 | N3 | 1.8367 | 1.1723 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Li1 |
C2 |
N3 |
59.478 |
|
Li1 |
N3 |
C2 |
87.167 |
| C2 |
Li1 |
N3 |
33.355 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.491 |
|
|
|
| 2 |
C |
-0.437 |
|
|
|
| 3 |
N |
-0.053 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
6.467 |
-2.472 |
0.000 |
6.923 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-6.278 |
-5.862 |
0.000 |
| y |
-5.862 |
-15.056 |
0.000 |
| z |
0.000 |
0.000 |
-14.333 |
|
| Traceless |
| | x | y | z |
| x |
8.417 |
-5.862 |
0.000 |
| y |
-5.862 |
-4.750 |
0.000 |
| z |
0.000 |
0.000 |
-3.666 |
|
| Polar |
| 3z2-r2 | -7.332 |
| x2-y2 | 8.778 |
| xy | -5.862 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.803 |
0.314 |
-0.000 |
| y |
0.314 |
3.769 |
-0.000 |
| z |
-0.000 |
-0.000 |
3.141 |
<r2> (average value of r
2) Å
2
| <r2> |
20.562 |
| (<r2>)1/2 |
4.535 |
Jump to
S1C1
S1C2
Energy calculated at PBE1PBE/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -100.279099 |
| Energy at 298.15K | -100.278034 |
| HF Energy | -100.279099 |
| Nuclear repulsion energy | 28.546539 |
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 PBE1PBE/aug-cc-pVTZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Σ |
2167 |
2083 |
173.38 |
|
|
|
| 2 |
Σ |
724 |
697 |
162.52 |
|
|
|
| 3 |
Π |
117 |
113 |
26.11 |
|
|
|
| 3 |
Π |
117 |
113 |
26.11 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1562.6 cm
-1
Scaled (by 0.9615) Zero Point Vibrational Energy (zpe) 1502.4 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at PBE1PBE/aug-cc-pVTZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
0.000 |
0.000 |
1.868 |
| C2 |
0.000 |
0.000 |
-1.062 |
| N3 |
0.000 |
0.000 |
0.109 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 2.9298 | 1.7586 |
C2 | 2.9298 | | 1.1712 | N3 | 1.7586 | 1.1712 | |
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 PBE1PBE/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.281 |
|
|
|
| 2 |
C |
-0.180 |
|
|
|
| 3 |
N |
-0.101 |
|
|
|
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 |
8.898 |
8.898 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.327 |
0.000 |
0.000 |
| y |
0.000 |
-14.327 |
0.000 |
| z |
0.000 |
0.000 |
-2.675 |
|
| Traceless |
| | x | y | z |
| x |
-5.826 |
0.000 |
0.000 |
| y |
0.000 |
-5.826 |
0.000 |
| z |
0.000 |
0.000 |
11.652 |
|
| Polar |
| 3z2-r2 | 23.305 |
| 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 |
3.206 |
0.000 |
0.000 |
| y |
0.000 |
3.206 |
0.000 |
| z |
0.000 |
0.000 |
4.695 |
<r2> (average value of r
2) Å
2
| <r2> |
23.839 |
| (<r2>)1/2 |
4.883 |