Fermi level movement for n- and p-GaAs interfaces: Effects of temperature and dopant concentration
Steven G. Anderson, C. M. Aldao, G. D. Waddill, I. M. Vitomirov, C. Capasso, J. H. Weaver
Abstract
Steven G. Anderson, C. M. Aldao, G. D. Waddill, I. M. Vitomirov, C. Capasso, J. H. Weaver
Abstract
Photoemission studies demonstrate that temperature and dopant concentration dependent movement of the surface Fermi level is controlled by coupling between adatom-induced and bulk states. At a low temperature for lightly doped n- or p-GaAs, initial band bending inhibits tunneling and EF remains near the band edges until the onset of metallicity. For heavy doping, greater band bending reflects a thinner depletion region. Thermal cycling for 20≤T≤300 K for low coverages demonstrates that band bending is reversible.
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Photoemission studies demonstrate that temperature and dopant concentration dependent movement of the surface Fermi level is controlled by coupling between adatom-induced and bulk states. At a low temperature for lightly doped n- or p-GaAs, initial band bending inhibits tunneling and EF remains near the band edges until the onset of metallicity. For heavy doping, greater band bending reflects a thinner depletion region. Thermal cycling for 20≤T≤300 K for low coverages demonstrates that band bending is reversible.
Key concepts: Band bending, Dopant, Fermi level, Doping, Condensed matter physics, Quantum tunnelling, Materials science, Chemistry