Jump to
S2C1
Energy calculated at B1B95/3-21G*
| | hartrees |
| Energy at 0K | -4134.848149 |
| Energy at 298.15K | -4134.847957 |
| HF Energy | -4134.848149 |
| Nuclear repulsion energy | 239.128875 |
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 B1B95/3-21G*
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 | | 2.2660 |
Ge2 | 2.2660 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/3-21G*
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 |
-38.369 |
0.000 |
0.000 |
| y |
0.000 |
-33.633 |
0.000 |
| z |
0.000 |
0.000 |
-32.033 |
|
| Traceless |
| | x | y | z |
| x |
-5.537 |
0.000 |
0.000 |
| y |
0.000 |
1.569 |
0.000 |
| z |
0.000 |
0.000 |
3.968 |
|
| Polar |
| 3z2-r2 | 7.936 |
| x2-y2 | -4.737 |
| 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 |
-1.117 |
0.000 |
0.000 |
| y |
0.000 |
5.411 |
0.000 |
| z |
0.000 |
0.000 |
15.498 |
<r2> (average value of r
2) Å
2
| <r2> |
103.819 |
| (<r2>)1/2 |
10.189 |
Jump to
S1C1
Energy calculated at B1B95/3-21G*
| | hartrees |
| Energy at 0K | -4134.827301 |
| Energy at 298.15K | -4134.827068 |
| HF Energy | -4134.827301 |
| Nuclear repulsion energy | 225.616015 |
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 B1B95/3-21G*
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Ge1 |
0.000 |
0.000 |
1.201 |
| Ge2 |
0.000 |
0.000 |
-1.201 |
Atom - Atom Distances (Å)
| |
Ge1 |
Ge2 |
| Ge1 | | 2.4018 |
Ge2 | 2.4018 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/3-21G*
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 |
-29.432 |
0.000 |
0.000 |
| y |
0.000 |
-38.956 |
0.000 |
| z |
0.000 |
0.000 |
-40.237 |
|
| Traceless |
| | x | y | z |
| x |
10.165 |
0.000 |
0.000 |
| y |
0.000 |
-4.122 |
0.000 |
| z |
0.000 |
0.000 |
-6.043 |
|
| Polar |
| 3z2-r2 | -12.086 |
| x2-y2 | 9.525 |
| 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 |
8.404 |
0.000 |
0.000 |
| y |
0.000 |
6.216 |
0.000 |
| z |
0.000 |
0.000 |
17.126 |
<r2> (average value of r
2) Å
2
| <r2> |
114.911 |
| (<r2>)1/2 |
10.720 |