Jump to
S1C2
Energy calculated at B3LYPultrafine/6-311G*
| hartrees |
Energy at 0K | -77.325410 |
Energy at 298.15K | -77.326379 |
HF Energy | -77.325410 |
Nuclear repulsion energy | 24.158556 |
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 B3LYPultrafine/6-311G*
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' |
677 |
654 |
0.00 |
|
|
|
2 |
A2" |
123 |
119 |
119.24 |
|
|
|
3 |
E' |
889 |
859 |
83.97 |
|
|
|
3 |
E' |
889 |
859 |
83.96 |
|
|
|
4 |
E' |
202 |
195 |
31.43 |
|
|
|
4 |
E' |
202 |
195 |
31.43 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1491.1 cm
-1
Scaled (by 0.9663) Zero Point Vibrational Energy (zpe) 1440.8 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 B3LYPultrafine/6-311G*
Point Group is D3h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.000 |
0.000 |
0.000 |
Li2 |
0.000 |
1.721 |
0.000 |
Li3 |
1.491 |
-0.861 |
0.000 |
Li4 |
-1.491 |
-0.861 |
0.000 |
Atom - Atom Distances (Å)
|
N1 |
Li2 |
Li3 |
Li4 |
N1 | | 1.7214 | 1.7214 | 1.7214 |
Li2 | 1.7214 | | 2.9816 | 2.9816 | Li3 | 1.7214 | 2.9816 | | 2.9816 | Li4 | 1.7214 | 2.9816 | 2.9816 | |
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 B3LYPultrafine/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-0.649 |
|
|
|
2 |
Li |
0.216 |
|
|
|
3 |
Li |
0.216 |
|
|
|
4 |
Li |
0.216 |
|
|
|
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 |
-3.461 |
0.000 |
0.000 |
y |
0.000 |
-3.461 |
0.000 |
z |
0.000 |
0.000 |
-22.193 |
|
Traceless |
| x | y | z |
x |
9.366 |
0.000 |
0.000 |
y |
0.000 |
9.366 |
0.000 |
z |
0.000 |
0.000 |
-18.732 |
|
Polar |
3z2-r2 | -37.464 |
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 |
18.567 |
0.000 |
0.000 |
y |
0.000 |
18.565 |
0.000 |
z |
0.000 |
0.000 |
20.377 |
<r2> (average value of r
2) Å
2
<r2> |
32.732 |
(<r2>)1/2 |
5.721 |
Jump to
S1C1
Energy calculated at B3LYPultrafine/6-311G*
| hartrees |
Energy at 0K | -77.325410 |
Energy at 298.15K | -77.326379 |
HF Energy | -77.325410 |
Nuclear repulsion energy | 24.160180 |
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 B3LYPultrafine/6-311G*
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 |
677 |
654 |
0.00 |
|
|
|
2 |
A1 |
123 |
119 |
119.30 |
|
|
|
3 |
E |
889 |
859 |
83.97 |
|
|
|
3 |
E |
889 |
859 |
83.96 |
|
|
|
4 |
E |
202 |
195 |
31.44 |
|
|
|
4 |
E |
202 |
195 |
31.44 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1491.2 cm
-1
Scaled (by 0.9663) Zero Point Vibrational Energy (zpe) 1441.0 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 B3LYPultrafine/6-311G*
Point Group is C3v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.000 |
0.000 |
0.001 |
Li2 |
0.000 |
1.721 |
-0.001 |
Li3 |
1.491 |
-0.861 |
-0.001 |
Li4 |
-1.491 |
-0.861 |
-0.001 |
Atom - Atom Distances (Å)
|
N1 |
Li2 |
Li3 |
Li4 |
N1 | | 1.7213 | 1.7213 | 1.7213 |
Li2 | 1.7213 | | 2.9814 | 2.9814 | Li3 | 1.7213 | 2.9814 | | 2.9814 | Li4 | 1.7213 | 2.9814 | 2.9814 | |
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 B3LYPultrafine/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-0.648 |
|
|
|
2 |
Li |
0.216 |
|
|
|
3 |
Li |
0.216 |
|
|
|
4 |
Li |
0.216 |
|
|
|
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 |
-0.006 |
0.006 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-3.462 |
0.000 |
0.000 |
y |
0.000 |
-3.462 |
0.000 |
z |
0.000 |
0.000 |
-22.192 |
|
Traceless |
| x | y | z |
x |
9.365 |
0.000 |
0.000 |
y |
0.000 |
9.365 |
0.000 |
z |
0.000 |
0.000 |
-18.730 |
|
Polar |
3z2-r2 | -37.460 |
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 |
18.563 |
0.000 |
0.000 |
y |
0.000 |
18.561 |
0.000 |
z |
0.000 |
0.000 |
20.372 |
<r2> (average value of r
2) Å
2
<r2> |
32.728 |
(<r2>)1/2 |
5.721 |