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Fizika i Tekhnika Poluprovodnikov, 2016 Volume 50, Issue 12, Pages 1629–1633 (Mi phts6283)

XX International Symposium ''Nanophysics and Nanoelectronics'', Nizhny Novgorod, March 14-18, 2016

On the radiative recombination and tunneling of charge carriers in SiGe/Si heterostructures with double quantum wells

A. N. Yablonskiia, R. Kh. Zhukavina, N. A. Bekina, A. V. Novikovba, D. V. Yurasova, M. V. Shaleeva

a Institute for Physics of Microstructures, Russian Academy of Sciences, Nizhnii Novgorod
b Lobachevsky State University of Nizhny Novgorod

Abstract: For SiGe/Si(001) epitaxial structures with two nonequivalent SiGe quantum wells separated by a thin Si barrier, the spectral and time characteristics of interband photoluminescence corresponding to the radiative recombination of excitons in quantum wells are studied. For a series of structures with two SiGe quantum wells different in width, the characteristic time of tunneling of charge carriers (holes) from the narrow quantum well, distinguished by a higher exciton recombination energy, to the wide quantum well is determined as a function of the Si barrier thickness. It is shown that the time of tunneling of holes between the Si$_{0.85}$Ge$_{0.15}$ layers with thicknesses of 3 and 9 nm steadily decreases from $\sim$500 to $<$ 5 ns, as the Si barrier thickness is reduced from 16 to 8 nm. At intermediate Si barrier thicknesses, an increase in the photoluminescence signal from the wide quantum well is observed, with a characteristic time of the same order of magnitude as the luminescence decay time of the narrow quantum well. This supports the observation of the effect of the tunneling of holes from the narrow to the wide quantum well. A strong dependence of the tunneling time of holes on the Ge content in the SiGe layers at the same thickness of the Si barrier between quantum wells is observed, which is attributed to an increase in the effective Si barrier height.

Received: 27.04.2016
Accepted: 10.05.2016


 English version:
Semiconductors, 2016, 50:12, 1604–1608

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