Jump to
S2C1
Energy calculated at HF/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -4157.373737 |
| Energy at 298.15K | |
| HF Energy | -4157.373737 |
| Nuclear repulsion energy | 209.663887 |
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 HF/6-311+G(3df,2p)
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Ga1 |
0.000 |
0.000 |
-1.331 |
| As2 |
0.000 |
0.000 |
1.251 |
Atom - Atom Distances (Å)
| |
Ga1 |
As2 |
| Ga1 | | 2.5820 |
As2 | 2.5820 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Ga |
0.272 |
|
|
|
| 2 |
As |
-0.272 |
|
|
|
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 |
-1.589 |
1.589 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-33.729 |
0.000 |
0.000 |
| y |
0.000 |
-33.729 |
0.000 |
| z |
0.000 |
0.000 |
-43.140 |
|
| Traceless |
| | x | y | z |
| x |
4.706 |
0.000 |
0.000 |
| y |
0.000 |
4.706 |
0.000 |
| z |
0.000 |
0.000 |
-9.411 |
|
| Polar |
| 3z2-r2 | -18.822 |
| x2-y2 | 0.000 |
| 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 |
11.616 |
0.000 |
0.000 |
| y |
0.000 |
11.616 |
0.000 |
| z |
0.000 |
0.000 |
17.342 |
<r2> (average value of r
2) Å
2
| <r2> |
129.588 |
| (<r2>)1/2 |
11.384 |
Jump to
S1C1
Energy calculated at HF/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -4157.312165 |
| Energy at 298.15K | |
| HF Energy | -4157.312165 |
| Nuclear repulsion energy | 210.925997 |
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 HF/6-311+G(3df,2p)
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Ga1 |
0.000 |
0.000 |
-1.323 |
| As2 |
0.000 |
0.000 |
1.243 |
Atom - Atom Distances (Å)
| |
Ga1 |
As2 |
| Ga1 | | 2.5665 |
As2 | 2.5665 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Ga |
0.224 |
|
|
|
| 2 |
As |
-0.224 |
|
|
|
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 |
-1.319 |
1.319 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-29.824 |
0.000 |
0.000 |
| y |
0.000 |
-38.961 |
0.000 |
| z |
0.000 |
0.000 |
-42.885 |
|
| Traceless |
| | x | y | z |
| x |
11.099 |
0.000 |
0.000 |
| y |
0.000 |
-2.607 |
0.000 |
| z |
0.000 |
0.000 |
-8.492 |
|
| Polar |
| 3z2-r2 | -16.985 |
| x2-y2 | 9.137 |
| 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 |
11.402 |
0.000 |
0.000 |
| y |
0.000 |
10.547 |
0.000 |
| z |
0.000 |
0.000 |
17.610 |
<r2> (average value of r
2) Å
2
| <r2> |
128.539 |
| (<r2>)1/2 |
11.338 |