1994
DOI: 10.1006/spmi.1994.1035
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Non-linear luminescence due to exciton - e-h plasma transformation in mixed type I - type II quantum wells

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Cited by 9 publications
(3 citation statements)
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“…We utilize [8] these properties in order to form a 2DEG with a controlled density in the wide wells by photoexciting with an Ar + laser, E L 2 = 2.41 eV and intensities at the sample surface of 0 ≤ I L 2 ≤ 8 mW cm 2 . In the PL experiments we simultaneously photoexcited the MTQW at E L 2 and just above the (e1: hh1) W 1S exciton band with a Ti:Sapphire laser at an energy of E L 1 = 1.538 eV and with a fixed intensity of I L 1 = 3 W cm 2 (cf.…”
Section: Methodsmentioning
confidence: 99%
“…We utilize [8] these properties in order to form a 2DEG with a controlled density in the wide wells by photoexciting with an Ar + laser, E L 2 = 2.41 eV and intensities at the sample surface of 0 ≤ I L 2 ≤ 8 mW cm 2 . In the PL experiments we simultaneously photoexcited the MTQW at E L 2 and just above the (e1: hh1) W 1S exciton band with a Ti:Sapphire laser at an energy of E L 1 = 1.538 eV and with a fixed intensity of I L 1 = 3 W cm 2 (cf.…”
Section: Methodsmentioning
confidence: 99%
“…The optical properties of quantum well (QW) structures, containing two-dimensional electron and hole gases (2DEG and 2DHG), have a scientific and technological importance [1,2]. The influence of those gases are studied in mixed types I-II quantum well (MTQW) structures, enabling the control of the electron density (n e ) between 10 10 -10 11 carriers cm −2 by optical pumping [4][5][6][7].…”
Section: Introductionmentioning
confidence: 99%
“…The influence of those gases are studied in mixed type I-type II quantum wells (MTQW) structure, enabling the control of the electron-density (he) between 1010_ 1011 carriers/cm2 by optical pumping [4][5][6][7].…”
Section: Introductionmentioning
confidence: 99%