Jump to
S2C1
Energy calculated at LSDA/3-21G
| hartrees |
Energy at 0K | -574.055711 |
Energy at 298.15K | -574.054307 |
Nuclear repulsion energy | 43.775671 |
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 LSDA/3-21G
Geometric Data calculated at LSDA/3-21G
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at LSDA/3-21G
| hartrees |
Energy at 0K | -574.178361 |
Energy at 298.15K | -574.177117 |
Nuclear repulsion energy | 50.952102 |
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 LSDA/3-21G
Point Group is D∞h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Si1 |
0.000 |
0.000 |
1.018 |
Si2 |
0.000 |
0.000 |
-1.018 |
Atom - Atom Distances (Å)
|
Si1 |
Si2 |
Si1 | | 2.0356 |
Si2 | 2.0356 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/3-21G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Si |
0.000 |
|
|
|
2 |
Si |
0.000 |
|
|
|
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 |
-29.109 |
0.000 |
0.000 |
y |
0.000 |
-29.109 |
0.000 |
z |
0.000 |
0.000 |
-18.144 |
|
Traceless |
| x | y | z |
x |
-5.483 |
0.000 |
0.000 |
y |
0.000 |
-5.483 |
0.000 |
z |
0.000 |
0.000 |
10.965 |
|
Polar |
3z2-r2 | 21.930 |
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 |
17.679 |
0.000 |
0.000 |
y |
0.000 |
17.679 |
0.000 |
z |
0.000 |
0.000 |
13.198 |
<r2> (average value of r
2) Å
2
<r2> |
44.904 |
(<r2>)1/2 |
6.701 |