TY - JOUR
T1 - Plasmons in coupled electron-hole double quantum wells
AU - Aizin, G. R.
AU - Laikhtman, B.
AU - Gumbs, Godfrey
PY - 2001
Y1 - 2001
N2 - We calculate the plasmon excitations in InAs/GaSb double quantum wells (QWs) coupled by tunneling. In this system the valence band of the GaSb layer overlaps with the conduction band of the InAs layer, and a tunneling gap is formed in the single particle energy spectrum due to the coupling between electrons in the InAs layer and holes in the GaSb layer. The plasmon spectrum is calculated within the random phase approximation for different positions of the Fermi level. We demonstrate that in general the plasmon spectrum consists of two branches, optical and acoustic. Both modes strongly depend on the position of the Fermi level. An optical mode exists for any position of the Fermi level above or below the tunneling gap. There is an acoustic mode only when the Fermi level is in the range of energies where the unperturbed electron and hole bands overlap, excluding the tunneling gap. When the Fermi level is positioned in the tunneling gap both modes disappear. This gap in the plasmon spectrum is unique for semimetallic InAs/GaSb double QWs and does not have any analog in the GaAs-based double QWs. The plasmon dispersion law and its dependence on the Fermi level position are analyzed numerically as well as analytically in the long wavelength limit, neglecting retardation effects.
AB - We calculate the plasmon excitations in InAs/GaSb double quantum wells (QWs) coupled by tunneling. In this system the valence band of the GaSb layer overlaps with the conduction band of the InAs layer, and a tunneling gap is formed in the single particle energy spectrum due to the coupling between electrons in the InAs layer and holes in the GaSb layer. The plasmon spectrum is calculated within the random phase approximation for different positions of the Fermi level. We demonstrate that in general the plasmon spectrum consists of two branches, optical and acoustic. Both modes strongly depend on the position of the Fermi level. An optical mode exists for any position of the Fermi level above or below the tunneling gap. There is an acoustic mode only when the Fermi level is in the range of energies where the unperturbed electron and hole bands overlap, excluding the tunneling gap. When the Fermi level is positioned in the tunneling gap both modes disappear. This gap in the plasmon spectrum is unique for semimetallic InAs/GaSb double QWs and does not have any analog in the GaAs-based double QWs. The plasmon dispersion law and its dependence on the Fermi level position are analyzed numerically as well as analytically in the long wavelength limit, neglecting retardation effects.
UR - http://www.scopus.com/inward/record.url?scp=0035883457&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.64.125317
DO - 10.1103/PhysRevB.64.125317
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AN - SCOPUS:0035883457
SN - 1098-0121
VL - 64
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 12
ER -