Jump to
S2C1
Energy calculated at B97D3/6-311G**
| | hartrees |
| Energy at 0K | -4155.948742 |
| Energy at 298.15K | -4155.948504 |
| HF Energy | -4155.948742 |
| Nuclear repulsion energy | 234.638430 |
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 B97D3/6-311G**
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Ge1 |
0.000 |
0.000 |
1.155 |
| Ge2 |
0.000 |
0.000 |
-1.155 |
Atom - Atom Distances (Å)
| |
Ge1 |
Ge2 |
| Ge1 | | 2.3094 |
Ge2 | 2.3094 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-311G**
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 |
-35.899 |
-2.688 |
0.000 |
| y |
-2.688 |
-35.902 |
0.000 |
| z |
0.000 |
0.000 |
-31.983 |
|
| Traceless |
| | x | y | z |
| x |
-1.957 |
-2.688 |
0.000 |
| y |
-2.688 |
-1.961 |
0.000 |
| z |
0.000 |
0.000 |
3.918 |
|
| Polar |
| 3z2-r2 | 7.836 |
| x2-y2 | 0.002 |
| xy | -2.688 |
| 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> |
106.941 |
| (<r2>)1/2 |
10.341 |
Jump to
S1C1
Energy calculated at B97D3/6-311G**
| | hartrees |
| Energy at 0K | -4155.911010 |
| Energy at 298.15K | -4155.910892 |
| HF Energy | -4155.911010 |
| Nuclear repulsion energy | 246.486803 |
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 B97D3/6-311G**
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Ge1 |
0.000 |
0.000 |
1.099 |
| Ge2 |
0.000 |
0.000 |
-1.099 |
Atom - Atom Distances (Å)
| |
Ge1 |
Ge2 |
| Ge1 | | 2.1984 |
Ge2 | 2.1984 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-311G**
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 |
-38.308 |
0.000 |
0.000 |
| y |
0.000 |
-28.829 |
0.000 |
| z |
0.000 |
0.000 |
-41.336 |
|
| Traceless |
| | x | y | z |
| x |
-3.226 |
0.000 |
0.000 |
| y |
0.000 |
10.993 |
0.000 |
| z |
0.000 |
0.000 |
-7.768 |
|
| Polar |
| 3z2-r2 | -15.536 |
| x2-y2 | -9.479 |
| 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> |
98.387 |
| (<r2>)1/2 |
9.919 |