Jump to
S1C2
Energy calculated at B1B95/6-31G**
| hartrees |
Energy at 0K | -413.313774 |
Energy at 298.15K | |
HF Energy | -413.313774 |
Nuclear repulsion energy | 25.488567 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Geometric Data calculated at B1B95/6-31G**
Point Group is D∞h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
S1 |
0.000 |
0.000 |
0.000 |
Li2 |
0.000 |
0.000 |
2.087 |
Li3 |
0.000 |
0.000 |
-2.087 |
Atom - Atom Distances (Å)
|
S1 |
Li2 |
Li3 |
S1 | | 2.0865 | 2.0865 |
Li2 | 2.0865 | | 4.1730 | Li3 | 2.0865 | 4.1730 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Li2 |
S1 |
Li3 |
180.000 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
S |
-0.480 |
|
|
|
2 |
Li |
0.240 |
|
|
|
3 |
Li |
0.240 |
|
|
|
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 |
-23.626 |
0.000 |
0.000 |
y |
0.000 |
-23.626 |
0.000 |
z |
0.000 |
0.000 |
12.590 |
|
Traceless |
| x | y | z |
x |
-18.108 |
0.000 |
0.000 |
y |
0.000 |
-18.108 |
0.000 |
z |
0.000 |
0.000 |
36.216 |
|
Polar |
3z2-r2 | 72.431 |
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 |
7.325 |
0.000 |
0.000 |
y |
0.000 |
7.325 |
0.000 |
z |
0.000 |
0.000 |
13.825 |
<r2> (average value of r
2) Å
2
<r2> |
33.338 |
(<r2>)1/2 |
5.774 |
Jump to
S1C1
Energy calculated at B1B95/6-31G**
| hartrees |
Energy at 0K | -413.314788 |
Energy at 298.15K | -413.315045 |
HF Energy | -413.314788 |
Nuclear repulsion energy | 25.437194 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Geometric Data calculated at B1B95/6-31G**
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
S1 |
0.000 |
0.000 |
0.258 |
Li2 |
0.000 |
1.877 |
-0.688 |
Li3 |
0.000 |
-1.877 |
-0.688 |
Atom - Atom Distances (Å)
|
S1 |
Li2 |
Li3 |
S1 | | 2.1019 | 2.1019 |
Li2 | 2.1019 | | 3.7543 | Li3 | 2.1019 | 3.7543 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Li2 |
S1 |
Li3 |
126.521 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
S |
-0.444 |
|
|
|
2 |
Li |
0.222 |
|
|
|
3 |
Li |
0.222 |
|
|
|
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 |
-4.944 |
4.944 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-23.781 |
0.000 |
0.000 |
y |
0.000 |
6.132 |
0.000 |
z |
0.000 |
0.000 |
-19.648 |
|
Traceless |
| x | y | z |
x |
-17.024 |
0.000 |
0.000 |
y |
0.000 |
27.847 |
0.000 |
z |
0.000 |
0.000 |
-10.823 |
|
Polar |
3z2-r2 | -21.646 |
x2-y2 | -29.914 |
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 |
8.006 |
0.000 |
0.000 |
y |
0.000 |
12.377 |
0.000 |
z |
0.000 |
0.000 |
8.586 |
<r2> (average value of r
2) Å
2
<r2> |
32.810 |
(<r2>)1/2 |
5.728 |