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S1C2
S1C3
Energy calculated at B2PLYP/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -100.290199 |
| Energy at 298.15K | -100.289192 |
| HF Energy | -100.177763 |
| Nuclear repulsion energy | 27.566347 |
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 B2PLYP/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 |
2168 |
2070 |
19.77 |
|
|
|
| 2 |
Σ |
636 |
607 |
108.14 |
|
|
|
| 3 |
Π |
148 |
141 |
36.91 |
|
|
|
| 3 |
Π |
148 |
141 |
36.91 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1549.6 cm
-1
Scaled (by 0.955) Zero Point Vibrational Energy (zpe) 1479.9 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 B2PLYP/6-31G(2df,p)
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
0.000 |
0.000 |
-2.059 |
| C2 |
0.000 |
0.000 |
-0.156 |
| N3 |
0.000 |
0.000 |
1.017 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 1.9028 | 3.0758 |
C2 | 1.9028 | | 1.1730 | N3 | 3.0758 | 1.1730 | |
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/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.193 |
|
|
|
| 2 |
C |
0.098 |
|
|
|
| 3 |
N |
-0.291 |
|
|
|
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 |
-8.755 |
8.755 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.199 |
0.000 |
0.000 |
| y |
0.000 |
-14.199 |
0.000 |
| z |
0.000 |
0.000 |
1.464 |
|
| Traceless |
| | x | y | z |
| x |
-7.831 |
0.000 |
0.000 |
| y |
0.000 |
-7.831 |
0.000 |
| z |
0.000 |
0.000 |
15.663 |
|
| Polar |
| 3z2-r2 | 31.325 |
| 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 |
2.702 |
0.000 |
0.000 |
| y |
0.000 |
2.702 |
0.000 |
| z |
0.000 |
0.000 |
4.199 |
<r2> (average value of r
2) Å
2
| <r2> |
25.710 |
| (<r2>)1/2 |
5.070 |
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S1C1
S1C3
Energy calculated at B2PLYP/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -100.297097 |
| Energy at 298.15K | -100.296365 |
| HF Energy | -100.186355 |
| Nuclear repulsion energy | 29.191645 |
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/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
1.436 |
-0.582 |
0.000 |
| C2 |
-0.718 |
-0.373 |
0.000 |
| N3 |
0.000 |
0.569 |
0.000 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 2.1647 | 1.8405 |
C2 | 2.1647 | | 1.1841 | N3 | 1.8405 | 1.1841 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Li1 |
C2 |
N3 |
58.212 |
|
Li1 |
N3 |
C2 |
88.636 |
| C2 |
Li1 |
N3 |
33.152 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.197 |
|
|
|
| 2 |
C |
-0.015 |
|
|
|
| 3 |
N |
-0.182 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
6.318 |
-2.394 |
0.000 |
6.756 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-5.889 |
-5.974 |
0.000 |
| y |
-5.974 |
-15.197 |
0.000 |
| z |
0.000 |
0.000 |
-14.579 |
|
| Traceless |
| | x | y | z |
| x |
8.999 |
-5.974 |
0.000 |
| y |
-5.974 |
-4.963 |
0.000 |
| z |
0.000 |
0.000 |
-4.036 |
|
| Polar |
| 3z2-r2 | -8.072 |
| x2-y2 | 9.308 |
| xy | -5.974 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.348 |
0.369 |
0.000 |
| y |
0.369 |
3.402 |
0.000 |
| z |
0.000 |
0.000 |
2.813 |
<r2> (average value of r
2) Å
2
| <r2> |
20.794 |
| (<r2>)1/2 |
4.560 |
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S1C1
S1C2
Energy calculated at B2PLYP/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -100.295818 |
| Energy at 298.15K | -100.294707 |
| HF Energy | -100.187322 |
| Nuclear repulsion energy | 28.325610 |
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/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 |
-1.070 |
| N3 |
0.000 |
0.000 |
0.113 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 2.9453 | 1.7621 |
C2 | 2.9453 | | 1.1831 | N3 | 1.7621 | 1.1831 | |
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/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.350 |
|
|
|
| 2 |
C |
-0.289 |
|
|
|
| 3 |
N |
-0.060 |
|
|
|
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 |
8.624 |
8.624 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.249 |
0.000 |
0.000 |
| y |
0.000 |
-14.249 |
0.000 |
| z |
0.000 |
0.000 |
-1.921 |
|
| Traceless |
| | x | y | z |
| x |
-6.164 |
0.000 |
0.000 |
| y |
0.000 |
-6.164 |
0.000 |
| z |
0.000 |
0.000 |
12.328 |
|
| Polar |
| 3z2-r2 | 24.656 |
| 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 |
2.655 |
0.000 |
0.000 |
| y |
0.000 |
2.655 |
0.000 |
| z |
0.000 |
0.000 |
4.236 |
<r2> (average value of r
2) Å
2
| <r2> |
23.842 |
| (<r2>)1/2 |
4.883 |