nextnano3 - Tutorial
next generation 3D nano device simulator
1D Tutorial
Solution of the Poisson equation for different charge density profiles
Note: This tutorial's copyright is owned by Stefan Birner,
www.nextnano.de.
Author:
Stefan Birner
Please send comments to nextnano3 (-at-) wsi.tum.de.
If you want to obtain the input files that are used within this tutorial, please contact stefan.birner@nextnano.de.
1) -> 1D_Poisson_dipole.in
2) -> 1D_Poisson_linear.in
3) -> 1D_Poisson_delta.in
1) Dipole: Constant charge density profile of positive and
negative charge
2) Linear charge density profile of positive and negative
charge
3) Delta-function like charge density profile of positive and
negative charges
The following figures show a dipole charge density distribution where
- the left region carries a constant positive
charge density (resulting from ionized donors ND+)
and
- the right region carries a constant negative charge density
(resulting from ionized acceptors NA-).
Left figure: 1Ddoping_concentration.dat
Right figure: densities1/density1Dspace_charge.dat

We have to solve the Poisson equation: d2phi / dx2
= - rho / (epsilon epsilon0)
The following figures shows the corresponding electric field distribution (left)
and the electrostatic potential (right).
Left figure: band_struc1/electric_field1D.dat
Right figure: band_struc1/potential1D.dat

The electric field is given by E(x) = - dphi / dx and
has a linear dependence (~ -x) because the electrostatic potential
has a quadratic dependence (~ x2).
The maximum value of the electric field is given by:
Emax = rho / (epsilon epsilon0) * x0 = e * 1*1018
cm-3 / ( 12.93 * 8.8542*10-12 As/Vm
) * 10 nm =
= 1.3995*107 V/m = 139.95
kV/cm
where x0 is the width of the positive (or negative) charge
density region, and epsilon = 12.93 is the static dielectric constant of GaAs.
The drop of the electrostatic potential between 0 nm and 20 nm is simply given
by the area that is below the graph of the electric field:
Delta phi = 1/2 Emax * 20 nm =
139.95 meV
The following figures show a linearly varying charge density distribution
where
- the left region carries a linearly decreasing
positive charge density (resulting from ionized donors
ND+) and
- the right region carries a linearly increasing negative
charge density (resulting from ionized acceptors NA-).
Left figure: 1Ddoping_concentration.dat
Right figure: densities1/density1Dspace_charge.dat

The following figures shows the corresponding electric field distribution (left)
and the electrostatic potential (right).
Left figure: band_struc1/electric_field1D.dat
Right figure: band_struc1/potential1D.dat

The electric field shows a quadratic dependence (~ -x2)
whereas the electrostatic potential shows a cubic dependence (~ x3).
The following figures show a delta-function like charge density distribution
where
- in the middle of the
structure there is a constant positive charge density of width
1 nm (resulting from ionized
donors ND+) and
- at the boundaries of the structure there are constant negative
charge densities of width 1 nm each (resulting from ionized acceptors NA-).
Left figure: 1Ddoping_concentration.dat
Right figure: densities1/density1Dspace_charge.dat

The following figures shows the corresponding electric field distribution (left)
and the electrostatic potential (right).
Left figure: band_struc1/electric_field1D.dat
Right figure: band_struc1/potential1D.dat

- Please help us to improve our tutorial. Send comments to
nextnano3
(-at-) wsi.tum.de.
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