Jump to
S2C1
Energy calculated at B1B95/6-311G**
| | hartrees |
| Energy at 0K | -4154.467026 |
| Energy at 298.15K | -4154.466823 |
| HF Energy | -4154.467026 |
| Nuclear repulsion energy | 239.070204 |
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 B1B95/6-311G**
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Ge1 |
0.000 |
0.000 |
1.133 |
| Ge2 |
0.000 |
0.000 |
-1.133 |
Atom - Atom Distances (Å)
| |
Ge1 |
Ge2 |
| Ge1 | | 2.2666 |
Ge2 | 2.2666 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G**
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 |
-33.543 |
0.000 |
0.000 |
| y |
0.000 |
-38.607 |
0.000 |
| z |
0.000 |
0.000 |
-32.036 |
|
| Traceless |
| | x | y | z |
| x |
1.779 |
0.000 |
0.000 |
| y |
0.000 |
-5.818 |
0.000 |
| z |
0.000 |
0.000 |
4.039 |
|
| Polar |
| 3z2-r2 | 8.078 |
| x2-y2 | 5.064 |
| 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 |
5.468 |
0.000 |
0.000 |
| y |
0.000 |
0.970 |
0.000 |
| z |
0.000 |
0.000 |
16.553 |
<r2> (average value of r
2) Å
2
| <r2> |
103.891 |
| (<r2>)1/2 |
10.193 |
Jump to
S1C1
Energy calculated at B1B95/6-311G**
| | hartrees |
| Energy at 0K | -4154.447692 |
| Energy at 298.15K | -4154.447440 |
| HF Energy | -4154.447692 |
| Nuclear repulsion energy | 224.802371 |
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 B1B95/6-311G**
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Ge1 |
0.000 |
0.000 |
1.205 |
| Ge2 |
0.000 |
0.000 |
-1.205 |
Atom - Atom Distances (Å)
| |
Ge1 |
Ge2 |
| Ge1 | | 2.4105 |
Ge2 | 2.4105 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G**
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 |
-39.330 |
0.000 |
0.000 |
| y |
0.000 |
-29.234 |
0.000 |
| z |
0.000 |
0.000 |
-40.299 |
|
| Traceless |
| | x | y | z |
| x |
-4.563 |
0.000 |
0.000 |
| y |
0.000 |
10.581 |
0.000 |
| z |
0.000 |
0.000 |
-6.017 |
|
| Polar |
| 3z2-r2 | -12.034 |
| x2-y2 | -10.096 |
| 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 |
6.227 |
0.000 |
0.000 |
| y |
0.000 |
7.872 |
0.000 |
| z |
0.000 |
0.000 |
18.855 |
<r2> (average value of r
2) Å
2
| <r2> |
115.630 |
| (<r2>)1/2 |
10.753 |