Jump to
S1C2
Energy calculated at wB97X-D/6-31+G**
| hartrees |
Energy at 0K | -77.265372 |
Energy at 298.15K | -77.266393 |
HF Energy | -77.265372 |
Nuclear repulsion energy | 23.915417 |
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 wB97X-D/6-31+G**
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' |
662 |
631 |
0.00 |
|
|
|
2 |
A2" |
138 |
131 |
124.23 |
|
|
|
3 |
E' |
879 |
837 |
122.43 |
|
|
|
3 |
E' |
879 |
837 |
122.26 |
|
|
|
4 |
E' |
216 |
205 |
35.56 |
|
|
|
4 |
E' |
216 |
205 |
35.35 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1494.6 cm
-1
Scaled (by 0.9523) Zero Point Vibrational Energy (zpe) 1423.3 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 wB97X-D/6-31+G**
Point Group is D3h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.000 |
0.000 |
0.000 |
Li2 |
0.000 |
1.730 |
0.000 |
Li3 |
1.498 |
-0.865 |
0.000 |
Li4 |
-1.498 |
-0.865 |
0.000 |
Atom - Atom Distances (Å)
|
N1 |
Li2 |
Li3 |
Li4 |
N1 | | 1.7299 | 1.7299 | 1.7299 |
Li2 | 1.7299 | | 2.9963 | 2.9963 | Li3 | 1.7299 | 2.9963 | | 2.9963 | Li4 | 1.7299 | 2.9963 | 2.9963 | |
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 wB97X-D/6-31+G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
0.206 |
|
|
|
2 |
Li |
-0.069 |
|
|
|
3 |
Li |
-0.069 |
|
|
|
4 |
Li |
-0.069 |
|
|
|
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 |
-2.654 |
0.000 |
0.000 |
y |
0.000 |
-2.654 |
0.000 |
z |
0.000 |
0.000 |
-22.860 |
|
Traceless |
| x | y | z |
x |
10.103 |
0.000 |
0.000 |
y |
0.000 |
10.103 |
0.000 |
z |
0.000 |
0.000 |
-20.206 |
|
Polar |
3z2-r2 | -40.412 |
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 |
18.126 |
0.000 |
0.000 |
y |
0.000 |
18.144 |
0.000 |
z |
0.000 |
0.000 |
20.598 |
<r2> (average value of r
2) Å
2
<r2> |
33.072 |
(<r2>)1/2 |
5.751 |
Jump to
S1C1
Energy calculated at wB97X-D/6-31+G**
| hartrees |
Energy at 0K | -77.265372 |
Energy at 298.15K | -77.266393 |
HF Energy | -77.265372 |
Nuclear repulsion energy | 23.915991 |
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 wB97X-D/6-31+G**
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 |
662 |
631 |
0.00 |
|
|
|
2 |
A1 |
138 |
131 |
124.25 |
|
|
|
3 |
E |
879 |
837 |
122.42 |
|
|
|
3 |
E |
879 |
837 |
122.26 |
|
|
|
4 |
E |
216 |
205 |
35.56 |
|
|
|
4 |
E |
216 |
205 |
35.35 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1494.7 cm
-1
Scaled (by 0.9523) Zero Point Vibrational Energy (zpe) 1423.4 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 wB97X-D/6-31+G**
Point Group is C3v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.000 |
0.000 |
0.082 |
Li2 |
0.000 |
1.731 |
-0.064 |
Li3 |
1.500 |
-0.866 |
-0.064 |
Li4 |
-1.500 |
-0.866 |
-0.064 |
Atom - Atom Distances (Å)
|
N1 |
Li2 |
Li3 |
Li4 |
N1 | | 1.7376 | 1.7376 | 1.7376 |
Li2 | 1.7376 | | 2.9990 | 2.9990 | Li3 | 1.7376 | 2.9990 | | 2.9990 | Li4 | 1.7376 | 2.9990 | 2.9990 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Li2 |
N1 |
Li3 |
119.306 |
|
Li2 |
N1 |
Li4 |
119.306 |
Li3 |
N1 |
Li4 |
119.306 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-31+G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
0.206 |
|
|
|
2 |
Li |
-0.069 |
|
|
|
3 |
Li |
-0.069 |
|
|
|
4 |
Li |
-0.069 |
|
|
|
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 |
-0.002 |
0.002 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-2.654 |
0.000 |
0.000 |
y |
0.000 |
-2.654 |
0.000 |
z |
0.000 |
0.000 |
-22.859 |
|
Traceless |
| x | y | z |
x |
10.103 |
0.000 |
0.000 |
y |
0.000 |
10.103 |
0.000 |
z |
0.000 |
0.000 |
-20.205 |
|
Polar |
3z2-r2 | -40.410 |
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 |
18.125 |
0.000 |
0.000 |
y |
0.000 |
18.143 |
0.000 |
z |
0.000 |
0.000 |
20.596 |
<r2> (average value of r
2) Å
2
<r2> |
33.071 |
(<r2>)1/2 |
5.751 |