Jump to
S1C2
Energy calculated at HF/LANL2DZ
| hartrees |
Energy at 0K | -76.732220 |
Energy at 298.15K | -76.733438 |
HF Energy | -76.732220 |
Nuclear repulsion energy | 23.677635 |
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/LANL2DZ
Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
1 |
A1' |
704 |
633 |
0.00 |
|
|
|
2 |
A2" |
188 |
170 |
189.67 |
|
|
|
3 |
E' |
907 |
816 |
249.60 |
|
|
|
3 |
E' |
907 |
816 |
249.60 |
|
|
|
4 |
E' |
249 |
224 |
71.40 |
|
|
|
4 |
E' |
249 |
224 |
71.40 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1601.7 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 1441.3 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 HF/LANL2DZ
Point Group is D3h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.000 |
0.000 |
0.000 |
Li2 |
0.000 |
1.756 |
0.000 |
Li3 |
1.521 |
-0.878 |
0.000 |
Li4 |
-1.521 |
-0.878 |
0.000 |
Atom - Atom Distances (Å)
|
N1 |
Li2 |
Li3 |
Li4 |
N1 | | 1.7564 | 1.7564 | 1.7564 |
Li2 | 1.7564 | | 3.0422 | 3.0422 | Li3 | 1.7564 | 3.0422 | | 3.0422 | Li4 | 1.7564 | 3.0422 | 3.0422 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Li2 |
N1 |
Li3 |
120.000 |
|
Li2 |
N1 |
Li4 |
120.000 |
Li3 |
N1 |
Li4 |
120.000 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-1.211 |
|
|
|
2 |
Li |
0.404 |
|
|
|
3 |
Li |
0.404 |
|
|
|
4 |
Li |
0.404 |
|
|
|
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 |
0.000 |
0.000 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-0.954 |
0.000 |
0.000 |
y |
0.000 |
-0.954 |
0.000 |
z |
0.000 |
0.000 |
-22.653 |
|
Traceless |
| x | y | z |
x |
10.849 |
0.000 |
0.000 |
y |
0.000 |
10.849 |
0.000 |
z |
0.000 |
0.000 |
-21.699 |
|
Polar |
3z2-r2 | -43.398 |
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 |
13.441 |
0.000 |
0.000 |
y |
0.000 |
13.441 |
0.000 |
z |
0.000 |
0.000 |
17.172 |
<r2> (average value of r
2) Å
2
<r2> |
32.878 |
(<r2>)1/2 |
5.734 |
Jump to
S1C1
Energy calculated at HF/LANL2DZ
| hartrees |
Energy at 0K | -76.732220 |
Energy at 298.15K | -76.733438 |
HF Energy | -76.732220 |
Nuclear repulsion energy | 23.675951 |
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/LANL2DZ
Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
1 |
A1 |
704 |
633 |
0.00 |
|
|
|
2 |
A1 |
189 |
170 |
189.57 |
|
|
|
3 |
E |
907 |
816 |
249.62 |
|
|
|
3 |
E |
907 |
816 |
249.62 |
|
|
|
4 |
E |
249 |
224 |
71.38 |
|
|
|
4 |
E |
249 |
224 |
71.38 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1601.5 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 1441.2 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 HF/LANL2DZ
Point Group is C3v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.000 |
0.000 |
-0.000 |
Li2 |
0.000 |
1.757 |
0.000 |
Li3 |
1.521 |
-0.878 |
0.000 |
Li4 |
-1.521 |
-0.878 |
0.000 |
Atom - Atom Distances (Å)
|
N1 |
Li2 |
Li3 |
Li4 |
N1 | | 1.7565 | 1.7565 | 1.7565 |
Li2 | 1.7565 | | 3.0424 | 3.0424 | Li3 | 1.7565 | 3.0424 | | 3.0424 | Li4 | 1.7565 | 3.0424 | 3.0424 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Li2 |
N1 |
Li3 |
120.000 |
|
Li2 |
N1 |
Li4 |
120.000 |
Li3 |
N1 |
Li4 |
120.000 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-1.211 |
|
|
|
2 |
Li |
0.404 |
|
|
|
3 |
Li |
0.404 |
|
|
|
4 |
Li |
0.404 |
|
|
|
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 |
0.001 |
0.001 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-0.953 |
0.000 |
0.000 |
y |
0.000 |
-0.953 |
0.000 |
z |
0.000 |
0.000 |
-22.655 |
|
Traceless |
| x | y | z |
x |
10.851 |
0.000 |
0.000 |
y |
0.000 |
10.851 |
0.000 |
z |
0.000 |
0.000 |
-21.702 |
|
Polar |
3z2-r2 | -43.404 |
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 |
13.444 |
0.000 |
0.000 |
y |
0.000 |
13.444 |
0.000 |
z |
0.000 |
0.000 |
17.177 |
<r2> (average value of r
2) Å
2
<r2> |
32.881 |
(<r2>)1/2 |
5.734 |