Jump to
S2C1
Energy calculated at LSDA/6-311G*
| | hartrees |
| Energy at 0K | -2473.638409 |
| Energy at 298.15K | -2473.635924 |
| Nuclear repulsion energy | 86.850963 |
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/6-311G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Se1 |
0.000 |
0.000 |
0.316 |
| O2 |
0.000 |
0.000 |
-1.342 |
Atom - Atom Distances (Å)
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Se |
0.334 |
|
|
|
| 2 |
O |
-0.334 |
|
|
|
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 |
2.067 |
2.067 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.802 |
0.000 |
0.000 |
| y |
0.000 |
-22.802 |
0.000 |
| z |
0.000 |
0.000 |
-24.008 |
|
| Traceless |
| | x | y | z |
| x |
0.603 |
0.000 |
0.000 |
| y |
0.000 |
0.603 |
0.000 |
| z |
0.000 |
0.000 |
-1.206 |
|
| Polar |
| 3z2-r2 | -2.412 |
| 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 |
2.302 |
0.000 |
0.000 |
| y |
0.000 |
2.302 |
0.000 |
| z |
0.000 |
0.000 |
4.438 |
<r2> (average value of r
2) Å
2
| <r2> |
0.000 |
| (<r2>)1/2 |
0.000 |
Jump to
S1C1
Energy calculated at LSDA/6-311G*
| | hartrees |
| Energy at 0K | -2473.598919 |
| Energy at 298.15K | -2473.596434 |
| Nuclear repulsion energy | 86.862388 |
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/6-311G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Se1 |
0.000 |
0.000 |
0.316 |
| O2 |
0.000 |
0.000 |
-1.341 |
Atom - Atom Distances (Å)
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Se |
0.344 |
|
|
|
| 2 |
O |
-0.344 |
|
|
|
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 |
2.111 |
2.111 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.507 |
0.000 |
0.000 |
| y |
0.000 |
-25.290 |
0.000 |
| z |
0.000 |
0.000 |
-24.126 |
|
| Traceless |
| | x | y | z |
| x |
4.201 |
0.000 |
0.000 |
| y |
0.000 |
-2.974 |
0.000 |
| z |
0.000 |
0.000 |
-1.227 |
|
| Polar |
| 3z2-r2 | -2.454 |
| x2-y2 | 4.783 |
| 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 |
2.183 |
0.000 |
0.000 |
| y |
0.000 |
2.413 |
0.000 |
| z |
0.000 |
0.000 |
4.220 |
<r2> (average value of r
2) Å
2
| <r2> |
32.340 |
| (<r2>)1/2 |
5.687 |