2005
DOI: 10.1016/j.ssc.2004.12.004
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Principal energy band gaps of the quaternary alloy AlxGa1−xSbyAs1−y

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Cited by 7 publications
(9 citation statements)
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“…Applying the tight-binding method to the same interface within the extended virtual crystal approximation which incorporates the compositional disorder, Rabeh et al [40] have found for E g the lawE g (x) = 0.705 + 0.895x + 0.486x 2 . A crossover from indirect to a direct band gap is observed at aluminum composition x = 0.45, which is in agreement with the results reported by [14] and [41].…”
Section: Resultssupporting
confidence: 92%
“…Applying the tight-binding method to the same interface within the extended virtual crystal approximation which incorporates the compositional disorder, Rabeh et al [40] have found for E g the lawE g (x) = 0.705 + 0.895x + 0.486x 2 . A crossover from indirect to a direct band gap is observed at aluminum composition x = 0.45, which is in agreement with the results reported by [14] and [41].…”
Section: Resultssupporting
confidence: 92%
“…While this constitutes a significant improvement over the bare GaSb buffer, the resistance is still not sufficient to isolate nanostructures as efficiently as a semi-insulating substrate. Sample C is comprised of an Al 0.35 Ga 0.65 Sb buffer that has a larger bandgap (1.2 eV [20]) but is not well lattice-matched (mismatch of 0.23%) in comparison with the GaSb buffer of Sample A. Sample D has a buffer made of the ternary alloy AlSb 0.91 As 0.09 that is characterized by a bandgap twice as large (2.4 eV [20]) and better lattice matching to GaSb (mismatch −0.1%) than Sample C. For these samples, Al 2 O 3 is used as dielectric to reduce the thermal budget during processing.…”
Section: Device Isolationmentioning
confidence: 99%
“…Sample C is comprised of an Al 0.35 Ga 0.65 Sb buffer that has a larger bandgap (1.2 eV [20]) but is not well lattice-matched (mismatch of 0.23%) in comparison with the GaSb buffer of Sample A. Sample D has a buffer made of the ternary alloy AlSb 0.91 As 0.09 that is characterized by a bandgap twice as large (2.4 eV [20]) and better lattice matching to GaSb (mismatch −0.1%) than Sample C. For these samples, Al 2 O 3 is used as dielectric to reduce the thermal budget during processing. Despite the nominally better intrinsic properties of these two buffer materials, we still measured a resistance of a few MΩs.…”
Section: Device Isolationmentioning
confidence: 99%
“…The lattice constant “a” varies linearly with composition (known as Vegard’s law). Accordingly, the lattice-matching conditions for quaternary alloys on a GaSb substrate can be written as follows [3,4]:AlxGa1normalxAsySb1normaly: y=0.0396x0.4426+0.0318x (0x1) GaxIn1normalxAsySb1normaly: y=0.38350.3835x0.4210+0.0216x (0x1)…”
Section: Introductionmentioning
confidence: 99%