1.4. Double Quantum Well¶
This tutorial calculates the energy eigenstates of a double quantum well. This aims to reproduce two figures (Figs. 3.16, 3.17, p. 92) of Paul Harrison’s excellent book “Quantum Wells, Wires and Dots” (Section 3.9 “The Double Quantum Well”), thus the following description is based on the explanations made therein. We are grateful that the book comes along with a CD so that we were able to look up the relevant material parameters and to check the results for consistency.
Input files for both the nextnano++ and nextnano³ software are available.
The following input file is used:
DoubleQuantumWell_6_nm_nn*.in
Structure: AlGaAs / 6nm GaAs / AlGaAs / 6nm AlGaAs / AlGaAs¶
Our symmetric double quantum well consists of two 6 nm GaAs quantum wells, separated by a Al_{0.2} Ga_{0.8} As barrier and surrounded by 20 nm Al_{0.2} Ga_{0.8} As barriers on each side. We thus have the following layer sequence: 20 nm Al_{0.2} Ga_{0.8} As / 6 nm GaAs / Al_{0.2} Ga_{0.8} As / 6 nm GaAs / 20 nm Al_{0.2} Ga_{0.8} As. (The barriers are printed in bold.)
In this tutorial, we demonstrate the following two examples:
we set the thickness of the Al_{0.2} Ga_{0.8} As barrier that separates the two quantum wells 4 nm and calculate the lowest two eigenstates.
we vary the thickness of the barrier layer from 1 nm to 14 nm fixing the width of the quantum well (6 nm). Then we calculate the lowest two eigenstates for each case and see the barrierwidth dependency of their eigenenergies.
We also explain where the relevant output files are in.
Material Parameters¶
The material parameters are given in database_nn*.in
but we can also redefine them manually in input files.
In this tutorial, we redefine parameters so that they are the same as the section 3.9 of Paul Harrison’s book “Quantum Wells, Wires and Dots”.
conduction band offset 
Al_{0.2} Ga_{0.52} As / GaAs 
0.167 eV 
conduction band effective mass 
Al_{0.2} Ga_{0.52} As 
0.084 m_{0} 
conduction band effective mass 
GaAs 
0.067 m_{0} 
Results¶
1. barrier width = 4 nm¶
The following figure shows the conduction band edge and wave functions that are confined inside the wells with barrier width = 4 nm.
(Note that the energies were shifted so that the conduction band edge of GaAs equals 0 eV.)
The wave functions form a symmetric and an antisymmetric pair. The symmetric one is lower in energy than the antisymmetric one. The plot is in excellent agreement with Fig. 3.17 (page 92) of Paul Harrison’s book “Quantum Wells, Wires and Dots”.
For comparison, the following figure shows for the same structure as above, the square of the wave function rather than \(\psi\) only.
Output¶
The conduction band edge of the Gamma conduction band can be found here:
bias_00000/bandedge_Gamma.dat (nextnano++)band_structure/cb_Gamma.dat (nextnano³)This file contains the eigenenergies of the two lowest eigenstates. The units are [eV].
bias_00000/Quantum/wf_energy_spectrum_quantum_region_Gamma_0000.dat (nextnano++)Schroedinger_1band/ev_cb1_sg1_deg1.dat (nextnano³)These are the comparison of eigenvalues:
nextnano++ 
nextnano³ 
Harrison’s book 

ground state energy [eV] 
0.04920 
0.04920 
0.04912 
first excited state energy [eV] 
0.05779 
0.05779 
0.05770 
This file contains the eigenenergies and the wave functions (\(\psi\)):
bias_00000/Quantum/wf_amplitudes_shift_quantum_region_Gamma_0000.dat (nextnano++)Schroedinger_1band/cb1_sg1_deg1_psi_shift.dat (nextnano³)This file contains the eigenenergies and the squared wave functions (\(\psi ^2\)):
bias_00000/Quantum/wf_probabilities_shift_quantum_region_Gamma_0000.dat (nextnano++)Schroedinger_1band/cb1_sg1_deg1_psi_squared_shift.dat (nextnano³)The subscript
_shift
indicates that \(\psi ^2\) and \(\psi\) are shifted by the corresponding energy levels.
and c. can be used to plot the data as shown in the figures above.
2. barrier width = 1 ~ 14 nm¶
Here, we varied the thickness of the Al_{0.2} Ga_{0.8} As barrier layer from 1 nm to 14 nm fixing the width of the quantum well (6 nm). We calculated the lowest two eigenstates and show their eigenvalues for each barrier width in the following figure.
If the separation between the two quantum wells is large, the wells behave as two independent single quantum wells having the identical ground state energies. The interaction between the energy levels localized within each well increases once the distance between the two wells decreases below 10 nm. One state is forced to higher energies and the other to lower energies. (Here, the electron spins align in an “antiparallel” arrangement in order to satisfy the Pauli exclusion principle.)
This is analogous to the hydrogen molecule where the formation of a pair of bonding and antibonding orbitals occurs once the two hydrogen atoms A and B are brought together.
\(\psi_{\rm bonding}\ \ \ \ \ \ \ =\ \frac{1}{\sqrt{2}} \psi_A\ +\ \psi_B\ \ \ \ \ \ \ \) (lower energy)\(\psi_{\rm antibonding}\ \ =\ \frac{1}{\sqrt{2}} \psi_A\ \ \psi_B\ \ \ \ \ \ \ \) (higher energy)Again, the plot is in excellent agreement with Fig. 3.16 (page 92) of Paul Harrison’s book “Quantum Wells, Wires and Dots”.
Output¶
The energy values were taken from the same file as before:
bias_00000/Quantum/wf_energy_spectrum_quantum_region_Gamma_0000.dat (nextnano++)Schredinger_1band/ev_cb1_sg1_deg1.dat (nextnano³)
For example, the values for the 1 nm barrier read:
nextnano++ 
nextnano³ 
Harrison’s book 

ground state energy [eV] 
0.03476 
0.03476 
0.03470 
first excited state energy [eV] 
0.07298 
0.07298 
0.07290 
The values for the 14 nm barrier read:
nextnano++ 
nextnano³ 
Harrison’s book 

ground state energy [eV] 
0.05332 
0.05332 
0.05323 
first excited state energy [eV] 
0.05338 
0.05338 
0.05329 
Tip: Sweeping¶
A sweep over the thickness of the Al_{0.2} Ga_{0.8} As barrier layer, i.e. the variable %QW_SEPARATION
, can easily be done by using nextnanomat’s Template feature.
The following screenshot shows how this can be done.
Go to “Template”, open input file, select “Range of values”, select “QW_SEPARATION”, click on “Create input files”, go to “Run and start your simulations.
Another tutorial on coupled quantum wells can be found here .