The tunneling mechanism of electrons and holes to surface states from near-surface Al0.3Ga0.7As/GaAs quantum wells has been investigated by steady-state and time-resolved photoluminescence spectroscopy, near liquid-helium temperature, of the excitonic e1-hh1 transition in the well. The ensemble of the data, taken over a wide range of optical excitation levels, for various values of the tunneling-barrier thickness, and before and after passivation of the surface by hydrogen, allows a description both of the details of the tunneling mechanism and of the character and behavior of relevant surface states. The main results are summarized as follows: (i) steady-state tunneling is ambipolar, namely, separate for electrons and holes, rather than excitonic; (ii) Spicer's advanced unified defect model for an oxidized GaAs surface, antisite-As donors as dominating surface trap's, provides an appropriate description of the state distribution at the interface between AlGaAs and its oxide; (iii) hole accumulation in surface states, resulting from the nominally different unipolar tunneling probability for the two carriers (and increasing with excitation level), generates a dipole electric field across the tunneling barrier, extending into the well; (iv) hydrogenation efficiently passivates electron trapping in surface states, but not hole tunneling and the consequent generation of a surface field by illumination; (v) the experimental findings agree with a model for ambipolar tunneling based on a self-consistent quantum-mechanical approach.

Emiliani, V., Bonanni, B., Presilla, C., Capizzi, M., Frova, A., Chang, Y.-., et al. (1994). Interaction mechanisms of near-surface quantum wells with oxidized and H-passivated AlGaAs surfaces. JOURNAL OF APPLIED PHYSICS, 75(10), 5114-5122 [10.1063/1.355757].

Interaction mechanisms of near-surface quantum wells with oxidized and H-passivated AlGaAs surfaces

Bonanni, B.;
1994-01-01

Abstract

The tunneling mechanism of electrons and holes to surface states from near-surface Al0.3Ga0.7As/GaAs quantum wells has been investigated by steady-state and time-resolved photoluminescence spectroscopy, near liquid-helium temperature, of the excitonic e1-hh1 transition in the well. The ensemble of the data, taken over a wide range of optical excitation levels, for various values of the tunneling-barrier thickness, and before and after passivation of the surface by hydrogen, allows a description both of the details of the tunneling mechanism and of the character and behavior of relevant surface states. The main results are summarized as follows: (i) steady-state tunneling is ambipolar, namely, separate for electrons and holes, rather than excitonic; (ii) Spicer's advanced unified defect model for an oxidized GaAs surface, antisite-As donors as dominating surface trap's, provides an appropriate description of the state distribution at the interface between AlGaAs and its oxide; (iii) hole accumulation in surface states, resulting from the nominally different unipolar tunneling probability for the two carriers (and increasing with excitation level), generates a dipole electric field across the tunneling barrier, extending into the well; (iv) hydrogenation efficiently passivates electron trapping in surface states, but not hole tunneling and the consequent generation of a surface field by illumination; (v) the experimental findings agree with a model for ambipolar tunneling based on a self-consistent quantum-mechanical approach.
1994
Pubblicato
Rilevanza internazionale
Articolo
Esperti anonimi
Settore FIS/03 - FISICA DELLA MATERIA
English
Emiliani, V., Bonanni, B., Presilla, C., Capizzi, M., Frova, A., Chang, Y.-., et al. (1994). Interaction mechanisms of near-surface quantum wells with oxidized and H-passivated AlGaAs surfaces. JOURNAL OF APPLIED PHYSICS, 75(10), 5114-5122 [10.1063/1.355757].
Emiliani, V; Bonanni, B; Presilla, C; Capizzi, M; Frova, A; Chang, Y-; Tan, I-; Merz, Jl; Colocci, M; Gurioli, M
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/2108/315479
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