Phase-shift analysis of two-dimensional carrier-carrier scattering in GaAs and GaN: Comparison with Born and classical approximations

Antónia Mošková and Martin Moško
Phys. Rev. B 61, 3048 – Published 15 January 2000
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Abstract

We study Markovian two-dimensional (2D) carrier-carrier (cc) scattering in GaAs and GaN quantum well systems. We evaluate the phase shifts of scattered partial waves by numerically solving the Schrödinger equation for the 2D cc collision problem. The output of this “phase shift analysis” is exact quantum results (in Markovian limit) for the 2D cc scattering cross section and 2D cc scattering rate. We compare these results with the results of the Born approximation (with the “Fermi-golden-rule based” theory), and find that the Born approximation can strongly overestimate the exact results. In particular, the 2D cc scattering rate is overestimated by a factor of 1 to 15 in the GaAs quantum well and by a factor of 2 to 100 in the GaN quantum well, if conditions typical for a quantum-well-laser device or for a quantum well excited by a short laser pulse are considered. Our study is performed for a statically screened intercarrier interaction, but we expect the dynamic screening to further deteriorate the Born approximation: We show that the weaker the screening the worse the Born approximation in a 2D system. We also analyze the 2D cc collision as a classical event, and find a very good agreement with the phase-shift analysis in the case of weak screening. For unscreened 2D cc collisions the hierarchy of exact, Born, and classical cross sections is derived analytically, and it is shown that the Born approximation breakdown is due to the carrier two dimensionality.

  • Received 30 December 1998

DOI:https://doi.org/10.1103/PhysRevB.61.3048

©2000 American Physical Society

Authors & Affiliations

Antónia Mošková and Martin Moško

  • Institute of Electrical Engineering, Slovak Academy of Sciences, Dúbravská cesta 9, SK-842 39 Bratislava, Slovak Republic

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Issue

Vol. 61, Iss. 4 — 15 January 2000

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