Jump to
S1C2
Energy calculated at HSEh1PBE/6-311G**
| hartrees |
Energy at 0K | -413.154510 |
Energy at 298.15K | -413.154248 |
HF Energy | -413.154510 |
Nuclear repulsion energy | 25.706388 |
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 HSEh1PBE/6-311G**
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 |
2.069 |
Li3 |
0.000 |
0.000 |
-2.069 |
Atom - Atom Distances (Å)
|
S1 |
Li2 |
Li3 |
S1 | | 2.0688 | 2.0688 |
Li2 | 2.0688 | | 4.1377 | Li3 | 2.0688 | 4.1377 | |
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 HSEh1PBE/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
S |
-1.030 |
|
|
|
2 |
Li |
0.515 |
|
|
|
3 |
Li |
0.515 |
|
|
|
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 |
-23.860 |
0.000 |
0.000 |
y |
0.000 |
-23.860 |
0.000 |
z |
0.000 |
0.000 |
13.346 |
|
Traceless |
| x | y | z |
x |
-18.603 |
0.000 |
0.000 |
y |
0.000 |
-18.603 |
0.000 |
z |
0.000 |
0.000 |
37.206 |
|
Polar |
3z2-r2 | 74.413 |
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 |
7.361 |
0.000 |
0.000 |
y |
0.000 |
7.361 |
0.000 |
z |
0.000 |
0.000 |
11.435 |
<r2> (average value of r
2) Å
2
<r2> |
32.837 |
(<r2>)1/2 |
5.730 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-311G**
| hartrees |
Energy at 0K | -413.154510 |
Energy at 298.15K | -413.154687 |
HF Energy | -413.154510 |
Nuclear repulsion energy | 25.705168 |
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 HSEh1PBE/6-311G**
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
S1 |
0.000 |
0.000 |
0.000 |
Li2 |
0.000 |
2.069 |
-0.001 |
Li3 |
0.000 |
-2.069 |
-0.001 |
Atom - Atom Distances (Å)
|
S1 |
Li2 |
Li3 |
S1 | | 2.0689 | 2.0689 |
Li2 | 2.0689 | | 4.1379 | Li3 | 2.0689 | 4.1379 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Li2 |
S1 |
Li3 |
179.946 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
S |
-1.030 |
|
|
|
2 |
Li |
0.515 |
|
|
|
3 |
Li |
0.515 |
|
|
|
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 |
-23.860 |
0.000 |
0.000 |
y |
0.000 |
13.349 |
0.000 |
z |
0.000 |
0.000 |
-23.860 |
|
Traceless |
| x | y | z |
x |
-18.605 |
0.000 |
0.000 |
y |
0.000 |
37.210 |
0.000 |
z |
0.000 |
0.000 |
-18.605 |
|
Polar |
3z2-r2 | -37.210 |
x2-y2 | -37.210 |
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 |
7.362 |
0.000 |
0.000 |
y |
0.000 |
11.437 |
0.000 |
z |
0.000 |
0.000 |
7.362 |
<r2> (average value of r
2) Å
2
<r2> |
32.839 |
(<r2>)1/2 |
5.731 |