Bilyovsкiy P. Effects of space redistribution of "hot" carriers sn semiconductors and heterostructures

Українська версія

Thesis for the degree of Candidate of Sciences (CSc)

State registration number

0410U005023

Applicant for

Specialization

  • 01.04.07 - Фізика твердого тіла

17-06-2010

Specialized Academic Board

Д 26.159.01

Institute of physics of NAS of Ukraine

Essay

The thesis is devoted to investigation of processes occurring with strongly non-equilibrium charge carriers in the bulk germanium crystals and n-InGaAs/GaAs heterostructures with quantum wells under the conditions of heating carriers by a high electric field. There have been studied instabilities arising under these conditions as well as formation of spatially non-uniform structures such as high-field domains or current filaments. Measurements of both the electric field distribution along a sample and infrared emission intensity revealed the thermal-diffusion autosolitons arising in the form of current filaments in the Ge crystals which were predicted earlier theoretically. There has been shown experimentally that such autosolitons arise in a weakly heated plasma with a high carrier concentration. In the case of plasma with a small carrier concentration and under strong heating up, the transverse autosolitons arise in the form of field domains. It is obtained that in the n-InGaAs/GaAs heterostructures with quantum wells under the lateral electric field, the static high field acoustoelectric domains may arise which cause the N-like behavior of their current-voltage characteristics. Using the double voltage pulse method, it is shown that decaying current oscillation, observed in the n-InGaAs/GaAs heterostructures, generated as a result of reflection of an acoustic flux by the anode contact. Also, it is shown that in the heterostructures with the double tunnel-coupled quantum wells a spatial transfer of heated electrons from the wider quantum wells into the narrower ones results in a sharp increase of intensity of the far infrared emission. An additional contribution of the direct radiative intersubband transitions of electrons in the narrower well can be responsible for this phenomenon.

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