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S1C2
S1C3
Energy calculated at B1B95/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -100.333407 |
| Energy at 298.15K | -100.332414 |
| HF Energy | -100.333407 |
| Nuclear repulsion energy | 27.736903 |
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 B1B95/6-31G(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 |
2272 |
2176 |
11.77 |
|
|
|
| 2 |
Σ |
640 |
613 |
111.01 |
|
|
|
| 3 |
Π |
152 |
145 |
36.75 |
|
|
|
| 3 |
Π |
152 |
145 |
36.75 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1607.8 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 1539.8 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 B1B95/6-31G(2df,p)
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
0.000 |
0.000 |
-2.056 |
| C2 |
0.000 |
0.000 |
-0.152 |
| N3 |
0.000 |
0.000 |
1.011 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 1.9049 | 3.0677 |
C2 | 1.9049 | | 1.1628 | N3 | 3.0677 | 1.1628 | |
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 B1B95/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.207 |
|
|
|
| 2 |
C |
0.135 |
|
|
|
| 3 |
N |
-0.342 |
|
|
|
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 |
-8.807 |
8.807 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.068 |
0.000 |
0.000 |
| y |
0.000 |
-14.068 |
0.000 |
| z |
0.000 |
0.000 |
1.639 |
|
| Traceless |
| | x | y | z |
| x |
-7.853 |
0.000 |
0.000 |
| y |
0.000 |
-7.853 |
0.000 |
| z |
0.000 |
0.000 |
15.707 |
|
| Polar |
| 3z2-r2 | 31.414 |
| 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 |
2.693 |
0.000 |
0.000 |
| y |
0.000 |
2.693 |
0.000 |
| z |
0.000 |
0.000 |
4.170 |
<r2> (average value of r
2) Å
2
| <r2> |
25.500 |
| (<r2>)1/2 |
5.050 |
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S1C1
S1C3
Energy calculated at B1B95/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -100.341163 |
| Energy at 298.15K | -100.340438 |
| HF Energy | -100.341163 |
| Nuclear repulsion energy | 29.377396 |
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 B1B95/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Li1 |
1.410 |
-0.615 |
0.000 |
| C2 |
-0.705 |
-0.365 |
0.000 |
| N3 |
0.000 |
0.577 |
0.000 |
Atom - Atom Distances (Å)
| |
Li1 |
C2 |
N3 |
| Li1 | | 2.1300 | 1.8462 |
C2 | 2.1300 | | 1.1768 | N3 | 1.8462 | 1.1768 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Li1 |
C2 |
N3 |
59.912 |
|
Li1 |
N3 |
C2 |
86.617 |
| C2 |
Li1 |
N3 |
33.472 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.220 |
|
|
|
| 2 |
C |
-0.007 |
|
|
|
| 3 |
N |
-0.213 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
6.261 |
-2.486 |
0.000 |
6.736 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-5.875 |
-5.965 |
0.000 |
| y |
-5.965 |
-14.910 |
0.000 |
| z |
0.000 |
0.000 |
-14.410 |
|
| Traceless |
| | x | y | z |
| x |
8.785 |
-5.965 |
0.000 |
| y |
-5.965 |
-4.767 |
0.000 |
| z |
0.000 |
0.000 |
-4.017 |
|
| Polar |
| 3z2-r2 | -8.034 |
| x2-y2 | 9.035 |
| xy | -5.965 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.313 |
0.367 |
0.000 |
| y |
0.367 |
3.390 |
0.000 |
| z |
0.000 |
0.000 |
2.782 |
<r2> (average value of r
2) Å
2
| <r2> |
20.540 |
| (<r2>)1/2 |
4.532 |
Jump to
S1C1
S1C2
Energy calculated at B1B95/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -100.339753 |
| Energy at 298.15K | |
| HF Energy | -100.339753 |
| Nuclear repulsion energy | 28.469214 |
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 B1B95/6-31G(2df,p)
Geometric Data calculated at B1B95/6-31G(2df,p)
Point Group is C∞v
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.387 |
|
|
|
| 2 |
C |
-0.314 |
|
|
|
| 3 |
N |
-0.073 |
|
|
|
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 |
9.038 |
9.038 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.083 |
0.000 |
0.000 |
| y |
0.000 |
-14.083 |
0.000 |
| z |
0.000 |
0.000 |
-0.738 |
|
| Traceless |
| | x | y | z |
| x |
-6.672 |
0.000 |
0.000 |
| y |
0.000 |
-6.672 |
0.000 |
| z |
0.000 |
0.000 |
13.345 |
|
| Polar |
| 3z2-r2 | 26.689 |
| 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 |
3.313 |
0.367 |
0.000 |
| y |
0.367 |
3.390 |
0.000 |
| z |
0.000 |
0.000 |
2.782 |
<r2> (average value of r
2) Å
2
| <r2> |
24.234 |
| (<r2>)1/2 |
4.923 |