2008
DOI: 10.1007/s11182-009-9177-8
|View full text |Cite
|
Sign up to set email alerts
|

Intermodulation of transverse magnetoresistance oscillations in structures with strong intersubband interaction

Abstract: In the Shubnikov-de Haas oscillation spectrum of doped InAs/AlSb structures, high-amplitude peaks are established at combination frequencies. It is demonstrated that they are caused by a significant contribution of intersubband scattering to the processes of electron-electron interaction.Keywords: two-dimensional electron gas, intra-and intersubband interaction of electrons, amplitude and frequency modulation of the Shubnikov-de Haas oscillations.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1

Citation Types

0
2
0

Year Published

2020
2020
2020
2020

Publication Types

Select...
1

Relationship

1
0

Authors

Journals

citations
Cited by 1 publication
(2 citation statements)
references
References 8 publications
0
2
0
Order By: Relevance
“…To confirm this assumption, let us present graphs of the dependences of the amplitude of the Shubnikov-de Haas oscillations on the inverse magnetic field [9,10]. The heterostructure AlSb( -Te)/InAs/( -Te)AlSb dynamics broadening of quantization depends on the scattering frequency DEG roughness heterojunction InAs/AlSb which is most intensively implemented at sites 1 and 2 (Fig.…”
Section: Overview Of the Quantum Intersubband Relaxation Time In The mentioning
confidence: 92%
See 1 more Smart Citation
“…To confirm this assumption, let us present graphs of the dependences of the amplitude of the Shubnikov-de Haas oscillations on the inverse magnetic field [9,10]. The heterostructure AlSb( -Te)/InAs/( -Te)AlSb dynamics broadening of quantization depends on the scattering frequency DEG roughness heterojunction InAs/AlSb which is most intensively implemented at sites 1 and 2 (Fig.…”
Section: Overview Of the Quantum Intersubband Relaxation Time In The mentioning
confidence: 92%
“…To solve the problem of taking into account the shielding effect, we use the first-order perturbation theory in the framework of the screening Lindhardt and expand on the potential of wave function where V is the volume studied structure generally and is the potential. By definition, the Fourier component k � −k is determined via the integral of the form (11) In linear approximation, induced charge is given by [9] where f k is the Fermi-Dirac equilibrium function. We introduce the replacement: q =k � −k,Q = (k � +k)∕2− which are the difference and the sum of the pulses, respectively.…”
Section: Theoretical Modelmentioning
confidence: 99%