Abstract:We have performed detailed optical measurements of ultrathin InAs/InP quantum wells grown by metal organic vapor phase epitaxy. Photoluminescence excitation spectra reveal the excitonic resonances associated with two- and three-monolayer thick InAs layers while polarization-dependent measurements clearly show the heavy- or light-hole nature of the resonances. These resonances, together with their emission bands, can be detected on the same sample, indicating the presence of well defined regions of different In… Show more
“…[3][4][5][6][7][8][9][10][11][12] However, the electronic states in ultrathin QWs are still not well understood. 3,6,10,11,15,16 The energy position of heavy-hole excitonic transitions deduced from the PL spectra can also be well reproduced by EFA. But EFA is highly questionable in the case of QWs which are only a few monolayers ͑ML͒ thick, 13 as indicated by recent tightbinding calculations on the InAs/GaAs system which depart significantly from the EFA approach.…”
“…[3][4][5][6][7][8][9][10][11][12] However, the electronic states in ultrathin QWs are still not well understood. 3,6,10,11,15,16 The energy position of heavy-hole excitonic transitions deduced from the PL spectra can also be well reproduced by EFA. But EFA is highly questionable in the case of QWs which are only a few monolayers ͑ML͒ thick, 13 as indicated by recent tightbinding calculations on the InAs/GaAs system which depart significantly from the EFA approach.…”
“…This shape difference is very well reproduced by the simulated spectra based on the Takagi-Taupin equations of the dynamical diffraction theory. According to calculations based on the envelope function approximation, 6,16,17 these energies can be made to correspond to heavy hole and light hole to electron transitions in 2 and 3 ML InAs quantum wells, respectively, provided that a conduction band gap offset ⌬Ec of 75% is used and an energy offset of 40 meV is added to the calculated values. Since the lattice parameter along the growth axis of InAs strained in InP is 6.26 Å, these thicknesses correspond to 1.88Ϯ0.15 and 2.78Ϯ0.15 ML, respectively.…”
Articles you may be interested inIn situ X-ray investigation of changing barrier growth temperatures on InGaN single quantum wells in metalorganic vapor phase epitaxy Ultrathin InAs/InP single quantum wells were grown by low-pressure metalorganic vapor phase epitaxy using tertiarybutylphosphine and tertiarybutylarsine, with nominal thicknesses between 2 and 3 ML. Characterization of a large number of samples by high-resolution x-ray diffraction ͑HR-XRD͒ and photoluminescence ͑PL͒ indicates an average InAs thickness very close to the nominal one. Photoluminescence excitation and absorption spectra of selected samples contain excitonic resonances associated with electron-hole transitions in 2 or 3 ML of InAs buried in InP. Only one set of these resonances appears in a given sample, thereby corroborating HR-XRD and PL measurements. Thus, our measurements indicate an absence of significant As-P intermixing.
“…The PLE spectra of peaks A1 and A2 are similar to what was previously reported in thin InAs QWs. 27,30 They show an edge at 1.19Ϯ 0.01 eV and a resonance at 1.31Ϯ 0.01 eV that correspond, respectively, to the electron to heavy-and light-hole transitions in a 2-ML-thick InAs/InP QW as calculated with the tight-binding method. 27,31 It follows that the high-energy tail of the emission from sample A at low temperature corresponds to residual emission from the WL.…”
We investigate the thermal quenching of the multimodal photoluminescence from InAs/InP (001) self-assembled quantum dots. The temperature evolution of the photoluminescence spectra of two samples is followed from 10 K to 300 K. We develop a coupled rate-equation model that includes the effect of carrier thermal escape from a quantum dot to the wetting layer and to the InP matrix, followed by transport, recapture or non-radiative recombination. Our model reproduces the temperature dependence of the emission of each family of quantum dots with a single set of parameters. We find that the main escape mechanism of the carriers confined in the quantum dots is through thermal emission to the wetting layer. The activation energy for this process is found to be close to one-half the energy difference between that of a given family of quantum dots and that of the wetting layer as measured by photoluminescence excitation experiments. This indicates that electron and holes exit the InAs quantum dots as correlated pairs.
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