Jump to
S2C1
Energy calculated at ROHF/6-311G*
| | hartrees |
| Energy at 0K | -4150.603153 |
| Energy at 298.15K | -4150.602950 |
| HF Energy | -4150.603153 |
| Nuclear repulsion energy | 230.179219 |
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 ROHF/6-311G*
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Ge1 |
0.000 |
0.000 |
1.177 |
| Ge2 |
0.000 |
0.000 |
-1.177 |
Atom - Atom Distances (Å)
| |
Ge1 |
Ge2 |
| Ge1 | | 2.3542 |
Ge2 | 2.3542 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROHF/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Ge |
0.000 |
|
|
|
| 2 |
Ge |
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 |
-34.717 |
0.000 |
0.000 |
| y |
0.000 |
-34.717 |
0.000 |
| z |
0.000 |
0.000 |
-42.353 |
|
| Traceless |
| | x | y | z |
| x |
3.818 |
0.000 |
0.000 |
| y |
0.000 |
3.818 |
0.000 |
| z |
0.000 |
0.000 |
-7.635 |
|
| Polar |
| 3z2-r2 | -15.271 |
| 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 |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
111.946 |
| (<r2>)1/2 |
10.580 |
Jump to
S1C1
Energy calculated at ROHF/6-311G*
| | hartrees |
| Energy at 0K | -4150.562758 |
| Energy at 298.15K | -4150.562538 |
| HF Energy | -4150.562758 |
| Nuclear repulsion energy | 226.772827 |
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 ROHF/6-311G*
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Ge1 |
0.000 |
0.000 |
1.195 |
| Ge2 |
0.000 |
0.000 |
-1.195 |
Atom - Atom Distances (Å)
| |
Ge1 |
Ge2 |
| Ge1 | | 2.3895 |
Ge2 | 2.3895 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROHF/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Ge |
0.000 |
|
|
|
| 2 |
Ge |
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 |
-40.763 |
0.000 |
0.000 |
| y |
0.000 |
-29.670 |
0.000 |
| z |
0.000 |
0.000 |
-42.375 |
|
| Traceless |
| | x | y | z |
| x |
-4.740 |
0.000 |
0.000 |
| y |
0.000 |
11.899 |
0.000 |
| z |
0.000 |
0.000 |
-7.158 |
|
| Polar |
| 3z2-r2 | -14.316 |
| x2-y2 | -11.093 |
| 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 |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
114.843 |
| (<r2>)1/2 |
10.716 |