Journal
NANOMATERIALS
Volume 11, Issue 2, Pages -Publisher
MDPI
DOI: 10.3390/nano11020468
Keywords
droplet density; droplet epitaxy; droplet etching; nucleation; scaling; rate model; Monte Carlo simulation
Categories
Funding
- Deutsche Forschungsgemeinschaft [HE 2466/2-1, HA 2042/8-1]
- European Union [721394]
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The temperature-dependent density of Al and Ga droplets on AlGaAs was studied theoretically, with successful simulation using two models. The critical nucleus size was found to depend on deposition time, contrary to the assumptions of the scaling model.
The temperature dependent density of Al and Ga droplets deposited on AlGaAs with molecular beam epitaxy is studied theoretically. Such droplets are important for applications in quantum information technology and can be functionalized e.g., by droplet epitaxy or droplet etching for the self-assembled generation of quantum emitters. After an estimation based on a scaling analysis, the droplet densities are simulated using first a mean-field rate model and second a kinetic Monte Carlo (KMC) simulation basing on an atomistic representation of the mobile adatoms. The modeling of droplet nucleation with a very high surface activity of the adatoms and ultra-low droplet densities down to 5 x 10(6) cm(-2) is highly demanding in particular for the KMC simulation. Both models consider two material related model parameters, the energy barrier ES for surface diffusion of free adatoms and the energy barrier EE for escape of atoms from droplets. The rate model quantitatively reproduces the droplet densities with ES = 0.19 eV, EE = 1.71 eV for Al droplets and ES = 0.115 eV for Ga droplets. For Ga, the values of EE are temperature dependent indicating the relevance of additional processes. Interestingly, the critical nucleus size depends on deposition time, which conflicts with the assumptions of the scaling model. Using a multiscale KMC algorithm to substantially shorten the computation times, Al droplets up to 460 degrees C on a 7500 x 7500 simulation field and Ga droplets up to 550 degrees C are simulated. The results show a very good agreement with the experiments using ES = 0.19 eV, EE = 1.44 eV for Al, and ES = 0.115 eV, EE = 1.24 eV (T <= 300 degrees C) or EE = 1.24 + 0.06 (T[degrees C] - 300)/100 eV (T>300 degrees C) for Ga. The deviating EE is attributed to a re-nucleation effect that is not considered in the mean-field assumption of the rate model.
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