Reproducible Science @ nanoHUB.org Reproducing DFT calculations in
Role of surface orientation on atomic layer deposited Al2O3/GaAs interface structure and Fermi level pinning
Ganesh Hegde, Gerhard Klimeck, and Alejandro Strachan Applied Physics Letters, 99, 093508 (2011)
Ale Strachan Network for Computational Nanotechnology (NCN) School of Materials Engineering
[email protected] The paper
Ale Strachan Key results
STEP 1 Used density functional theory (DFT) to predict atomic structure after 1st monolayer of Al2O3 is deposited on GaAs (111)A and (111)B surfaces Ga terminated As terminated
STEP 2 Computed their electronic density of states of resulting structures. Kohn-Sham eigenvalues (underestimate band-gap but trends should be accurate)
Main results • (111) B interface (blue line) exhibits electronic states within the band-gap • (111) A interface (black line) leads to no electronic states within the band-gap and some near the valence band maximum • Good agreement with MOSFET experiments that exhibit large currents when built on (111) A with little Fermi level pinning and no current in (111) B devices Ale Strachan M. Xu, et al. Electron Devices Meeting (IEDM), 2009 IEEE pp. 1–4. 3 The simulation tool
From the tools menu launch “nanoMATERIALS SeqQest DFT”
About the tool: SeqQuest, a density functional theory (DFT) code from Sandia National Laboratories: http://dft.sandia.gov/Quest/
Learn more: • Designing meaningful density functional theory calculations in materials science— a primer, Mattsson, et al. Modelling Simul. Mater. Sci. Eng. 13, R1-31 (2004). • nanoHUB-U course “Atoms to Materials” https://nanohub.org/courses/FATM
Ale Strachan 4 What we will do
Objective We will compute the electronic density of states of the (111)A and (111)B interfaces from the paper
Approach • We will select the appropriate structures • Perform a density functional theory electronic calculation using the generalized gradient approximation (GGA) • Analyze the electronic density of states for both configurations using Kohn-Sham eigenvalues
Ale Strachan 5 Specify the input structure
From the dropdown menu select GaAs-111A
You can check the atomic positions and cell parameters to be used in the calculation The cell is periodic along the a and b directions and open along the normal direction
Ale Strachan 6 Specify simulation details
Select GGA as the exchange and correlation functional
Specify 0.1 eV as the width of the Gaussian smearing to be used to plot the electronic density of states. Each Kohn-Sham eigenvalue will be replaced by a Gaussian with this standard deviation.
Ale Strachan 7 Finish setup and run
No need to compute forces on atoms
This simulations takes a while, about 20 minutes, go read about DFT of SeqQuest and come back… Submit the run
Ale Strachan 8 Visualizing the DoS
From the dropdown menu in the output select “Density of States”
Change the plot ranges: Click on the x and y axes select Manual • For x (electron energy) we will plot from -6 to -3 eV (the Fermi energy falls in this range – see next slide) • For y (DoS) we will plot from 0 to 5
Ale Strachan 9 Visualizing the DoS
To find out where the Fermi energy lies, plot the electron occupation statistics
Ale Strachan 10 Simulating the (111)B case
1. Without deleting the run, go back to the input to run the other interface
2. Select the (111) B interface
3. Re-select GGA and 0.05 eV for the DoS broadening
4. Click Simulate
Ale Strachan 11 Make a publication quality plot
You can visualize the results of both simulations at the same time
An make a publication quality plot directly from nanoHUB
You can customize your plot with line colors, symbols, fonts, sizes, etc.
Ale Strachan 12 Compare with predictions
nanoHUB result
• Similar trends in both DoS calculations, with (111)B interface showing significant states in the gap and the (111) A states near the conduction band edge • Possible reasons for discrepancy: different numerical values in k-points and real- space grid, differences in basis sets and pseudopotentials
Ale Strachan 13 Further work
• Explore the role of in-plane strain on the atomic and electronic structure of the two interfaces in the paper
• Study other semiconductor/oxide interfaces
Ale Strachan 14