Jump to
S1C2
Energy calculated at B3PW91/6-311G*
| hartrees |
Energy at 0K | -77.264417 |
Energy at 298.15K | -77.265348 |
HF Energy | -77.264417 |
Nuclear repulsion energy | 24.117076 |
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 B3PW91/6-311G*
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' |
674 |
649 |
0.00 |
|
|
|
2 |
A2" |
103 |
99 |
109.16 |
|
|
|
3 |
E' |
885 |
852 |
82.06 |
|
|
|
3 |
E' |
885 |
852 |
81.92 |
|
|
|
4 |
E' |
202 |
195 |
28.91 |
|
|
|
4 |
E' |
202 |
195 |
28.94 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1475.1 cm
-1
Scaled (by 0.9627) Zero Point Vibrational Energy (zpe) 1420.1 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 B3PW91/6-311G*
Point Group is D3h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.000 |
0.000 |
0.000 |
Li2 |
0.000 |
1.724 |
0.000 |
Li3 |
1.493 |
-0.862 |
0.000 |
Li4 |
-1.493 |
-0.862 |
0.000 |
Atom - Atom Distances (Å)
|
N1 |
Li2 |
Li3 |
Li4 |
N1 | | 1.7244 | 1.7244 | 1.7244 |
Li2 | 1.7244 | | 2.9867 | 2.9867 | Li3 | 1.7244 | 2.9867 | | 2.9867 | Li4 | 1.7244 | 2.9867 | 2.9867 | |
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 B3PW91/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-0.656 |
|
|
|
2 |
Li |
0.219 |
|
|
|
3 |
Li |
0.219 |
|
|
|
4 |
Li |
0.219 |
|
|
|
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 |
-2.974 |
0.000 |
0.000 |
y |
0.000 |
-2.974 |
0.000 |
z |
0.000 |
0.000 |
-21.914 |
|
Traceless |
| x | y | z |
x |
9.470 |
0.000 |
0.000 |
y |
0.000 |
9.470 |
0.000 |
z |
0.000 |
0.000 |
-18.940 |
|
Polar |
3z2-r2 | -37.879 |
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 |
18.693 |
0.000 |
0.000 |
y |
0.000 |
18.734 |
0.000 |
z |
0.000 |
0.000 |
20.709 |
<r2> (average value of r
2) Å
2
<r2> |
32.562 |
(<r2>)1/2 |
5.706 |
Jump to
S1C1
Energy calculated at B3PW91/6-311G*
| hartrees |
Energy at 0K | -77.264417 |
Energy at 298.15K | -77.265347 |
HF Energy | -77.264417 |
Nuclear repulsion energy | 24.120099 |
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 B3PW91/6-311G*
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 |
674 |
649 |
0.00 |
|
|
|
2 |
A1 |
102 |
99 |
109.27 |
|
|
|
3 |
E |
885 |
852 |
82.06 |
|
|
|
3 |
E |
885 |
852 |
81.93 |
|
|
|
4 |
E |
202 |
195 |
28.93 |
|
|
|
4 |
E |
202 |
195 |
28.96 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1475.3 cm
-1
Scaled (by 0.9627) Zero Point Vibrational Energy (zpe) 1420.3 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 B3PW91/6-311G*
Point Group is C3v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.000 |
0.000 |
0.001 |
Li2 |
0.000 |
1.724 |
-0.001 |
Li3 |
1.493 |
-0.862 |
-0.001 |
Li4 |
-1.493 |
-0.862 |
-0.001 |
Atom - Atom Distances (Å)
|
N1 |
Li2 |
Li3 |
Li4 |
N1 | | 1.7242 | 1.7242 | 1.7242 |
Li2 | 1.7242 | | 2.9864 | 2.9864 | Li3 | 1.7242 | 2.9864 | | 2.9864 | Li4 | 1.7242 | 2.9864 | 2.9864 | |
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 B3PW91/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-0.656 |
|
|
|
2 |
Li |
0.219 |
|
|
|
3 |
Li |
0.219 |
|
|
|
4 |
Li |
0.219 |
|
|
|
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 |
-0.009 |
0.009 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-2.976 |
0.000 |
0.000 |
y |
0.000 |
-2.976 |
0.000 |
z |
0.000 |
0.000 |
-21.911 |
|
Traceless |
| x | y | z |
x |
9.468 |
0.000 |
0.000 |
y |
0.000 |
9.468 |
0.000 |
z |
0.000 |
0.000 |
-18.935 |
|
Polar |
3z2-r2 | -37.871 |
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 |
18.686 |
0.000 |
0.000 |
y |
0.000 |
18.726 |
-0.001 |
z |
0.000 |
-0.001 |
20.699 |
<r2> (average value of r
2) Å
2
<r2> |
32.556 |
(<r2>)1/2 |
5.706 |