Jump to
S2C1
Energy calculated at HSEh1PBE/6-31G**
| | hartrees |
| Energy at 0K | -4149.245601 |
| Energy at 298.15K | -4149.245402 |
| HF Energy | -4149.245601 |
| Nuclear repulsion energy | 241.730659 |
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/6-31G**
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Ge1 |
0.000 |
0.000 |
1.121 |
| Ge2 |
0.000 |
0.000 |
-1.121 |
Atom - Atom Distances (Å)
| |
Ge1 |
Ge2 |
| Ge1 | | 2.2417 |
Ge2 | 2.2417 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-31G**
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 |
-33.478 |
0.000 |
0.000 |
| y |
0.000 |
-38.287 |
0.000 |
| z |
0.000 |
0.000 |
-32.112 |
|
| Traceless |
| | x | y | z |
| x |
1.722 |
0.000 |
0.000 |
| y |
0.000 |
-5.493 |
0.000 |
| z |
0.000 |
0.000 |
3.771 |
|
| Polar |
| 3z2-r2 | 7.542 |
| x2-y2 | 4.810 |
| 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 |
5.930 |
0.000 |
0.000 |
| y |
0.000 |
-0.804 |
0.000 |
| z |
0.000 |
0.000 |
15.454 |
<r2> (average value of r
2) Å
2
| <r2> |
102.027 |
| (<r2>)1/2 |
10.101 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-31G**
| | hartrees |
| Energy at 0K | -4149.221202 |
| Energy at 298.15K | -4149.220948 |
| HF Energy | -4149.221202 |
| Nuclear repulsion energy | 226.511313 |
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/6-31G**
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Ge1 |
0.000 |
0.000 |
1.196 |
| Ge2 |
0.000 |
0.000 |
-1.196 |
Atom - Atom Distances (Å)
| |
Ge1 |
Ge2 |
| Ge1 | | 2.3923 |
Ge2 | 2.3923 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-31G**
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 |
-29.237 |
0.000 |
0.000 |
| y |
0.000 |
-38.925 |
0.000 |
| z |
0.000 |
0.000 |
-40.408 |
|
| Traceless |
| | x | y | z |
| x |
10.429 |
0.000 |
0.000 |
| y |
0.000 |
-4.103 |
0.000 |
| z |
0.000 |
0.000 |
-6.326 |
|
| Polar |
| 3z2-r2 | -12.652 |
| x2-y2 | 9.688 |
| 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 |
9.077 |
0.000 |
0.000 |
| y |
0.000 |
7.077 |
0.000 |
| z |
0.000 |
0.000 |
17.254 |
<r2> (average value of r
2) Å
2
| <r2> |
114.171 |
| (<r2>)1/2 |
10.685 |