Jump to
S2C1
Energy calculated at HSEh1PBE/cc-pVDZ
| | hartrees |
| Energy at 0K | -4153.340871 |
| Energy at 298.15K | -4153.340667 |
| HF Energy | -4153.340871 |
| Nuclear repulsion energy | 238.127205 |
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/cc-pVDZ
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Ge1 |
0.000 |
0.000 |
1.138 |
| Ge2 |
0.000 |
0.000 |
-1.138 |
Atom - Atom Distances (Å)
| |
Ge1 |
Ge2 |
| Ge1 | | 2.2756 |
Ge2 | 2.2756 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/cc-pVDZ
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 |
-38.337 |
0.000 |
0.000 |
| y |
0.000 |
-33.493 |
0.000 |
| z |
0.000 |
0.000 |
-31.952 |
|
| Traceless |
| | x | y | z |
| x |
-5.614 |
0.000 |
0.000 |
| y |
0.000 |
1.652 |
0.000 |
| z |
0.000 |
0.000 |
3.963 |
|
| Polar |
| 3z2-r2 | 7.925 |
| x2-y2 | -4.844 |
| 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 |
1.549 |
0.000 |
0.000 |
| y |
0.000 |
5.156 |
0.000 |
| z |
0.000 |
0.000 |
15.763 |
<r2> (average value of r
2) Å
2
| <r2> |
104.459 |
| (<r2>)1/2 |
10.221 |
Jump to
S1C1
Energy calculated at HSEh1PBE/cc-pVDZ
| | hartrees |
| Energy at 0K | -4153.319208 |
| Energy at 298.15K | -4153.318953 |
| HF Energy | -4153.319208 |
| Nuclear repulsion energy | 223.749138 |
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/cc-pVDZ
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Ge1 |
0.000 |
0.000 |
1.211 |
| Ge2 |
0.000 |
0.000 |
-1.211 |
Atom - Atom Distances (Å)
| |
Ge1 |
Ge2 |
| Ge1 | | 2.4218 |
Ge2 | 2.4218 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/cc-pVDZ
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 |
-38.907 |
0.000 |
0.000 |
| y |
0.000 |
-29.143 |
0.000 |
| z |
0.000 |
0.000 |
-40.100 |
|
| Traceless |
| | x | y | z |
| x |
-4.285 |
0.000 |
0.000 |
| y |
0.000 |
10.361 |
0.000 |
| z |
0.000 |
0.000 |
-6.075 |
|
| Polar |
| 3z2-r2 | -12.150 |
| x2-y2 | -9.764 |
| 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 |
5.705 |
0.000 |
0.000 |
| y |
0.000 |
7.567 |
0.000 |
| z |
0.000 |
0.000 |
17.542 |
<r2> (average value of r
2) Å
2
| <r2> |
116.359 |
| (<r2>)1/2 |
10.787 |