2016
DOI: 10.1007/s11082-016-0667-y
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Photoluminescence quenching mechanisms in type II InAs/GaInSb QWs on InAs substrates

Abstract: Optical properties of AlSb/InAs/GaInSb/InAs/AlSb quantum wells (QWs) grown on an InAs substrate were investigated from the point of view of room temperature emission in the mid-and long-wavelength infrared ranges. By means of two independent techniques of optical spectroscopy, photoreflectance and temperature-dependent photoluminescence, it was proven that the main process limiting the performance of such InAs substrate-based type II structures is related to the escape of carriers from the hole ground state of… Show more

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Cited by 8 publications
(6 citation statements)
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“…This is consistent with the presence of intrinsic Ga Sb antisite defects reported in the GaAsSb system [9,34] and additionally, in NWs the Sb distribution is inhomogeneous both axially [9] and radially [14]. Hence, the origin of PL intensity quenching at higher temperatures (>100 K) in as-grown NWs could be assigned to the native defect-related non-radiative channels, as also reported by Dysik et al [34] in InAs/GaInSb type-II quantum wells. Figure 3(c) shows the RT Raman spectra of as-grown and annealed GaAsSb NWs.…”
Section: Resultssupporting
confidence: 89%
See 1 more Smart Citation
“…This is consistent with the presence of intrinsic Ga Sb antisite defects reported in the GaAsSb system [9,34] and additionally, in NWs the Sb distribution is inhomogeneous both axially [9] and radially [14]. Hence, the origin of PL intensity quenching at higher temperatures (>100 K) in as-grown NWs could be assigned to the native defect-related non-radiative channels, as also reported by Dysik et al [34] in InAs/GaInSb type-II quantum wells. Figure 3(c) shows the RT Raman spectra of as-grown and annealed GaAsSb NWs.…”
Section: Resultssupporting
confidence: 89%
“…The second larger value activation energy, E b , of 80 meV falls in the range of 60-120 meV commonly ascribed to lattice defects consisting of Ga Sb antisite defects and a complex related to Ga-vacancies [33]. This is consistent with the presence of intrinsic Ga Sb antisite defects reported in the GaAsSb system [9,34] and additionally, in NWs the Sb distribution is inhomogeneous both axially [9] and radially [14]. Hence, the origin of PL intensity quenching at higher temperatures (>100 K) in as-grown NWs could be assigned to the native defect-related non-radiative channels, as also reported by Dysik et al [34] in InAs/GaInSb type-II quantum wells.…”
Section: Resultssupporting
confidence: 77%
“…It is well known that in ternary III-V NW material alloy systems, inhomogeneous composition and phase separation [7], atomic ordering [8], and miscibility gap [9] phenomena can have deleterious effects on electrical and optical properties for NW devices operating at room temperature (RT). In the GaAsSb material system, in particular in the NW configuration, the electronic and the optoelectronic properties are strongly dependent on Sb concentration due to its inhomogeneous distribution in NWs both axially and radially [10], and also on the presence of point defects such as intrinsic Ga Sb antisite defects and Ga vacancies [11,12].…”
Section: Introductionmentioning
confidence: 99%
“…The PL temperature dependences were fitted by the Arrhenius-type plots (see e.g. [40,41]) to identify possible additional channels of non-radiative recombination, appearing at higher temperatures, and determine their activation energies. In case of j thermally activated non-radiative recombination processes responsible for the PL quenching, the temperature dependence of the normalized PL intensity, I PL (T), can be described by the following relation [42]…”
Section: Temperature Dependences Of the Mid-ir Plmentioning
confidence: 99%