1995
DOI: 10.1103/physrevb.51.7029
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Recombination processes and photoluminescence intensity in quantum wells under steady-state and transient conditions

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Cited by 22 publications
(17 citation statements)
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“…We neglect Auger processes, excitonic recombination ͑which may be important in the low-temperature regime͒, nonradiative recombination with interface traps ͑which may be relevant in the low-laser-intensity regime and at high temperatures͒, spatial diffusion, and drift. [7][8][9][10][11][12][13][14][15][16][17][18][19] In the following, we work within the effective-mass approximation and the parabolic-band model for describing both electrons and holes; for simplicity, we consider one hole band with a spherical carrier effective mass m v ϭ0.3m 0 , with m 0 being the free-electron mass, which results in a bulk value of 26 meV for the acceptor binding energy, in agreement with experiment. 20 Moreover, we limit ourselves to radiative recombination of nϭ1 conduction subband electrons with either free holes at the nϭ1 valence subband or with bound holes at neutral acceptors homogeneously distributed within the GaAs-͑Ga,Al͒As QWW.…”
Section: Theoretical Modelmentioning
confidence: 78%
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“…We neglect Auger processes, excitonic recombination ͑which may be important in the low-temperature regime͒, nonradiative recombination with interface traps ͑which may be relevant in the low-laser-intensity regime and at high temperatures͒, spatial diffusion, and drift. [7][8][9][10][11][12][13][14][15][16][17][18][19] In the following, we work within the effective-mass approximation and the parabolic-band model for describing both electrons and holes; for simplicity, we consider one hole band with a spherical carrier effective mass m v ϭ0.3m 0 , with m 0 being the free-electron mass, which results in a bulk value of 26 meV for the acceptor binding energy, in agreement with experiment. 20 Moreover, we limit ourselves to radiative recombination of nϭ1 conduction subband electrons with either free holes at the nϭ1 valence subband or with bound holes at neutral acceptors homogeneously distributed within the GaAs-͑Ga,Al͒As QWW.…”
Section: Theoretical Modelmentioning
confidence: 78%
“…11 The experimental data by Ding et al 10 and Bongiovanni and Staehli 11 were analyzed in a detailed study by Oliveira and de Dios-Leyva 12 on the steady-state PL of GaAs-͑Ga,Al͒As QW's. In a recent work, Brandt et al 13 presented a theoretical and experimental study of recombination processes and PL intensity in QW's under steady-state and transient conditions.…”
Section: Introductionmentioning
confidence: 99%
“…225 This is a well-established approach for characterizing complex, multiprocess recombination dynamics in bulk and nanostructured materials. 34,322,323 Experimental I em versus I exc along with results from the fitting routine are shown in Figure 31B. Individual trapped electron and continuum carrier concentrations at various I exc are displayed in Figure 31C.…”
Section: Recombination Mechanismsmentioning
confidence: 98%
“…As we observe a change in the radiative lifetime, we can rule out that the increase of the PL intensity is induced by an enhanced exciton generation rate due to the altered surface, since the excitonic radiative lifetime does not depend on the generation rate. 27 Two important points have to be stressed in this context: ͑i͒ Electrical measurements on NWs with exceptionally large diameters ͑d = 200 nm͒ did not yield any detectable current indicating complete depletion. The alignment of the conduction and valence bands across the NW diameter can be obtained by solving the Poisson equation in cylindrical geometry.…”
mentioning
confidence: 99%