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Fizika i Tekhnika Poluprovodnikov, 2010 Volume 44, Issue 8, Pages 1084–1092 (Mi phts8895)

This article is cited in 4 papers

Amorphous, glassy, porous, organic, microcrystalline semiconductors, semiconductor composites

InGaAs tunnel-injection structures with nanobridges: Excitation transfer and luminescence kinetics

V. G. Talalaevab, A. V. Senicheva, B. V. Novikova, J. W. Tommc, T. Elsaesserc, N. D. Zakharovd, P. Wernerd, U. Göseled, Yu. B. Samsonenkoefg, G. È. Cirlinefg

a V. A. Fock Institute of Physics, Saint-Petersburg State University
b Martin–Luther–Universität, ZIK "SiLi-nano", 06120 Halle, Deutschland
c Max–Born–Institut für Nichtlineare Optik und Kurzzeitspektroskopie, 12489 Berlin, Deutschland
d Max–Planck–Institut für Mikrostrukturphysik, 06120 Halle (Saale), Deutschland
e Ioffe Institute, St. Petersburg
f Institute for Analytical Instrumentation, Russian Academy of Sciences, St. Petersburg
g St. Petersburg Physical Technological Center for Research and Education, Russian Academy of Sciences, St. Petersburg, 195220, Russia

Abstract: Methods of optical spectroscopy and electron microscopy have been used to study tunnel-injection nanostructures the active region of which consisted of an upper In$_{0.15}$Ga$_{0.85}$As quantum-well layer and a lower layer of In$_{0.6}$Ga$_{0.4}$As quantum dots as a light emitter; both layers were separated by a GaAs barrier layer. Deviations from the semiclassical Wentzel–Kramers–Brillouin model are observed in the dependence of the tunneling time on barrier’s thickness. Reduction of the transfer time to several picoseconds at a barrier thickness smaller than 6 nm is accounted for by formation of InGaAs nanobridges between tops of quantum dots and the quantum-well layer; the nanobridges include those with their own hole state. The effect of an electric field induced by tunneling on the carriers’ transfer time in a tunnel-injection nanostructure is taken into account.

Received: 28.12.2009
Accepted: 11.01.2010


 English version:
Semiconductors, 2010, 44:8, 1050–1058

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