2000
DOI: 10.1116/1.591460
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Molecular beam epitaxy of PbSrSe and PbSe/PbSrSe multiple quantum well structures for use in midinfrared light emitting devices

Abstract: PbSrSe layers and PbSe/PbSrSe multiple quantum well (MQW) structures have been grown on BaF2 (111) substrates by molecular beam epitaxy. The lattice constant of the PbSrSe alloy was determined by x-ray diffraction, and both the refractive index and absorption edge of the PbSrSe alloy with Sr composition up to 0.23 were obtained from Fourier transform infrared transmission spectra at room temperature. MQW structures exhibit strong photoluminescence (PL) in the 3–5 μm wavelength range at room temperature. The PL… Show more

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Cited by 28 publications
(28 citation statements)
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References 14 publications
(10 reference statements)
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“…Such designs are now an integral part of mid-IR and THz QCL fabrication where a three-level energy structure is created with the bottom two energies spaced by 36 meV, the LO phonon energy of the GaAs QW material [1,29]. The total band gap difference for this QW is 177 meV, which is close to the room temperature band gap difference of 173 meV between the PbSe (E g =278 meV) well and Pb 0.93 Sr 0.07 Se (E g =451 meV) barrier materials used in prior experimental studies [21][22][23][24][25][26][27]. This allows rapid filling of the upper laser transition state along with rapid emptying of the bottom laser transition state thus helping to reduce further the threshold for population inversion.…”
Section: Iv-vi Quantum Well Materialsmentioning
confidence: 86%
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“…Such designs are now an integral part of mid-IR and THz QCL fabrication where a three-level energy structure is created with the bottom two energies spaced by 36 meV, the LO phonon energy of the GaAs QW material [1,29]. The total band gap difference for this QW is 177 meV, which is close to the room temperature band gap difference of 173 meV between the PbSe (E g =278 meV) well and Pb 0.93 Sr 0.07 Se (E g =451 meV) barrier materials used in prior experimental studies [21][22][23][24][25][26][27]. This allows rapid filling of the upper laser transition state along with rapid emptying of the bottom laser transition state thus helping to reduce further the threshold for population inversion.…”
Section: Iv-vi Quantum Well Materialsmentioning
confidence: 86%
“…Depending on alloy composition and temperature, their bandgaps range from 0 to over 500 meV. Detailed procedures for growth and characterization of PbSrSe/PbSe MQWs on (111)-oriented BaF 2 and silicon have been described elsewhere [21][22][23][24][25][26]. The bands are almost mirror images of each other, see Table II, so similar quantum effects are expected in both the conduction and valence bands.…”
Section: Iv-vi Quantum Well Materialsmentioning
confidence: 99%
“…They are strained by 0.16% due to the slightly different lattice constants of PbSe and Pb 0.93 Sr 0.07 Se (Ref. 16).…”
Section: Layer Setupmentioning
confidence: 99%
“…IV–VI QWs have been successfully fabricated with growth directions along 〈111〉, 〈100〉, and 〈110〉 11, 14, 15. For QWs grown along [111] direction, the four‐valley degenerate at four L points splits into one longitudinal and three oblique branches.…”
Section: Physical Model and Mathematical Formulationmentioning
confidence: 99%