Jump to
S1C2
Energy calculated at B3LYP/cc-pVTZ
| hartrees |
Energy at 0K | -77.332469 |
Energy at 298.15K | -77.333463 |
HF Energy | -77.332469 |
Nuclear repulsion energy | 24.227272 |
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 B3LYP/cc-pVTZ
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' |
681 |
658 |
0.00 |
|
|
|
2 |
A2" |
126 |
121 |
136.99 |
|
|
|
3 |
E' |
895 |
865 |
81.89 |
|
|
|
3 |
E' |
895 |
865 |
81.93 |
|
|
|
4 |
E' |
204 |
197 |
33.29 |
|
|
|
4 |
E' |
204 |
197 |
33.27 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1501.8 cm
-1
Scaled (by 0.9666) Zero Point Vibrational Energy (zpe) 1451.6 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 B3LYP/cc-pVTZ
Point Group is D3h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.000 |
0.000 |
0.000 |
Li2 |
0.000 |
1.717 |
0.000 |
Li3 |
1.487 |
-0.858 |
0.000 |
Li4 |
-1.487 |
-0.858 |
0.000 |
Atom - Atom Distances (Å)
|
N1 |
Li2 |
Li3 |
Li4 |
N1 | | 1.7165 | 1.7165 | 1.7165 |
Li2 | 1.7165 | | 2.9731 | 2.9731 | Li3 | 1.7165 | 2.9731 | | 2.9731 | Li4 | 1.7165 | 2.9731 | 2.9731 | |
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 B3LYP/cc-pVTZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
0.060 |
|
|
|
2 |
Li |
-0.020 |
|
|
|
3 |
Li |
-0.020 |
|
|
|
4 |
Li |
-0.020 |
|
|
|
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 |
-3.150 |
0.000 |
0.000 |
y |
0.000 |
-3.150 |
0.000 |
z |
0.000 |
0.000 |
-22.339 |
|
Traceless |
| x | y | z |
x |
9.595 |
0.000 |
0.000 |
y |
0.000 |
9.595 |
0.000 |
z |
0.000 |
0.000 |
-19.189 |
|
Polar |
3z2-r2 | -38.378 |
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 |
18.346 |
0.000 |
0.000 |
y |
0.000 |
18.362 |
0.000 |
z |
0.000 |
0.000 |
19.852 |
<r2> (average value of r
2) Å
2
<r2> |
32.481 |
(<r2>)1/2 |
5.699 |
Jump to
S1C1
Energy calculated at B3LYP/cc-pVTZ
| hartrees |
Energy at 0K | -77.332469 |
Energy at 298.15K | -77.333463 |
HF Energy | -77.332469 |
Nuclear repulsion energy | 24.228612 |
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 B3LYP/cc-pVTZ
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 |
681 |
658 |
0.00 |
|
|
|
2 |
A1 |
125 |
121 |
137.03 |
|
|
|
3 |
E |
895 |
865 |
81.89 |
|
|
|
3 |
E |
895 |
865 |
81.92 |
|
|
|
4 |
E |
204 |
197 |
33.30 |
|
|
|
4 |
E |
204 |
197 |
33.27 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1501.9 cm
-1
Scaled (by 0.9666) Zero Point Vibrational Energy (zpe) 1451.7 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 B3LYP/cc-pVTZ
Point Group is C3v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.000 |
0.000 |
0.001 |
Li2 |
0.000 |
1.716 |
-0.001 |
Li3 |
1.486 |
-0.858 |
-0.001 |
Li4 |
-1.486 |
-0.858 |
-0.001 |
Atom - Atom Distances (Å)
|
N1 |
Li2 |
Li3 |
Li4 |
N1 | | 1.7165 | 1.7165 | 1.7165 |
Li2 | 1.7165 | | 2.9730 | 2.9730 | Li3 | 1.7165 | 2.9730 | | 2.9730 | Li4 | 1.7165 | 2.9730 | 2.9730 | |
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 B3LYP/cc-pVTZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
0.060 |
|
|
|
2 |
Li |
-0.020 |
|
|
|
3 |
Li |
-0.020 |
|
|
|
4 |
Li |
-0.020 |
|
|
|
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 |
-0.007 |
0.007 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-3.151 |
0.000 |
0.000 |
y |
0.000 |
-3.151 |
0.000 |
z |
0.000 |
0.000 |
-22.338 |
|
Traceless |
| x | y | z |
x |
9.594 |
0.000 |
0.000 |
y |
0.000 |
9.594 |
0.000 |
z |
0.000 |
0.000 |
-19.187 |
|
Polar |
3z2-r2 | -38.375 |
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 |
18.343 |
0.000 |
0.000 |
y |
0.000 |
18.359 |
-0.000 |
z |
0.000 |
-0.000 |
19.849 |
<r2> (average value of r
2) Å
2
<r2> |
32.479 |
(<r2>)1/2 |
5.699 |