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S1C2
S1C3
Energy calculated at B3PW91/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -100.328116 |
| Energy at 298.15K | -100.327122 |
| HF Energy | -100.328116 |
| Nuclear repulsion energy | 27.668579 |
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 B3PW91/6-31G(2df,p)
| 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 |
2248 |
2161 |
12.24 |
|
|
|
| 2 |
Σ |
630 |
606 |
109.98 |
|
|
|
| 3 |
Π |
153 |
147 |
37.04 |
|
|
|
| 3 |
Π |
153 |
147 |
37.04 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1592.0 cm
-1
Scaled (by 0.9614) Zero Point Vibrational Energy (zpe) 1530.5 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 B3PW91/6-31G(2df,p)
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
0.000 |
0.000 |
-2.060 |
| C2 |
0.000 |
0.000 |
-0.153 |
| N3 |
0.000 |
0.000 |
1.014 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 1.9070 | 3.0732 |
C2 | 1.9070 | | 1.1662 | N3 | 3.0732 | 1.1662 | |
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 B3PW91/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.207 |
|
|
|
| 2 |
C |
0.136 |
|
|
|
| 3 |
N |
-0.343 |
|
|
|
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 |
-8.801 |
8.801 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.078 |
0.000 |
0.000 |
| y |
0.000 |
-14.078 |
0.000 |
| z |
0.000 |
0.000 |
1.651 |
|
| Traceless |
| | x | y | z |
| x |
-7.865 |
0.000 |
0.000 |
| y |
0.000 |
-7.865 |
0.000 |
| z |
0.000 |
0.000 |
15.729 |
|
| Polar |
| 3z2-r2 | 31.459 |
| 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 |
2.719 |
0.000 |
0.000 |
| y |
0.000 |
2.719 |
0.000 |
| z |
0.000 |
0.000 |
4.207 |
<r2> (average value of r
2) Å
2
| <r2> |
25.576 |
| (<r2>)1/2 |
5.057 |
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S1C1
S1C3
Energy calculated at B3PW91/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -100.334800 |
| Energy at 298.15K | -100.334056 |
| HF Energy | -100.334800 |
| Nuclear repulsion energy | 29.266197 |
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 B3PW91/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
1.437 |
-0.583 |
0.000 |
| C2 |
-0.719 |
-0.369 |
0.000 |
| N3 |
0.000 |
0.566 |
0.000 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 2.1665 | 1.8406 |
C2 | 2.1665 | | 1.1796 | N3 | 1.8406 | 1.1796 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Li1 |
C2 |
N3 |
58.147 |
|
Li1 |
N3 |
C2 |
88.871 |
| C2 |
Li1 |
N3 |
32.982 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.228 |
|
|
|
| 2 |
C |
-0.021 |
|
|
|
| 3 |
N |
-0.207 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
6.368 |
-2.402 |
0.000 |
6.806 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-5.686 |
-5.932 |
0.000 |
| y |
-5.932 |
-15.017 |
0.000 |
| z |
0.000 |
0.000 |
-14.414 |
|
| Traceless |
| | x | y | z |
| x |
9.029 |
-5.932 |
0.000 |
| y |
-5.932 |
-4.967 |
0.000 |
| z |
0.000 |
0.000 |
-4.062 |
|
| Polar |
| 3z2-r2 | -8.124 |
| x2-y2 | 9.331 |
| xy | -5.932 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.355 |
0.384 |
0.000 |
| y |
0.384 |
3.407 |
0.000 |
| z |
0.000 |
0.000 |
2.820 |
<r2> (average value of r
2) Å
2
| <r2> |
20.678 |
| (<r2>)1/2 |
4.547 |
Jump to
S1C1
S1C2
Energy calculated at B3PW91/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -100.333864 |
| Energy at 298.15K | -100.332756 |
| HF Energy | -100.333864 |
| Nuclear repulsion energy | 28.397418 |
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 B3PW91/6-31G(2df,p)
| 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 |
2155 |
2071 |
161.14 |
|
|
|
| 2 |
Σ |
733 |
704 |
139.73 |
|
|
|
| 3 |
Π |
105 |
101 |
25.48 |
|
|
|
| 3 |
Π |
105 |
101 |
25.48 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1548.4 cm
-1
Scaled (by 0.9614) Zero Point Vibrational Energy (zpe) 1488.6 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 B3PW91/6-31G(2df,p)
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 |
-1.067 |
| N3 |
0.000 |
0.000 |
0.111 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 2.9419 | 1.7633 |
C2 | 2.9419 | | 1.1786 | N3 | 1.7633 | 1.1786 | |
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 B3PW91/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.369 |
|
|
|
| 2 |
C |
-0.288 |
|
|
|
| 3 |
N |
-0.082 |
|
|
|
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 |
8.626 |
8.626 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.117 |
0.000 |
0.000 |
| y |
0.000 |
-14.117 |
0.000 |
| z |
0.000 |
0.000 |
-1.769 |
|
| Traceless |
| | x | y | z |
| x |
-6.174 |
0.000 |
0.000 |
| y |
0.000 |
-6.174 |
0.000 |
| z |
0.000 |
0.000 |
12.348 |
|
| Polar |
| 3z2-r2 | 24.695 |
| 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 |
2.672 |
0.000 |
0.000 |
| y |
0.000 |
2.672 |
0.000 |
| z |
0.000 |
0.000 |
4.234 |
<r2> (average value of r
2) Å
2
| <r2> |
23.710 |
| (<r2>)1/2 |
4.869 |