2016
DOI: 10.1016/j.spmi.2015.12.034
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Electrical performance of InAs/AlSb/GaSb superlattice photodetectors

Abstract: a b s t r a c tTemperature dependence of dark current measurements is an efficient way to verify the quality of an infrared detector. Low dark current density values are needed for high performance detector applications. Identification of dominant current mechanisms in each operating temperature can be used to extract minority carrier lifetimes which are highly important for understanding carrier transport and improving the detector performance. InAs/AlSb/GaSb based T2SL N-structures with AlSb unipolar barrier… Show more

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Cited by 13 publications
(5 citation statements)
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“…Figure 5 shows the current-voltage curves of the ICIP-2 at different temperatures. The dark current density at −0.05 V is as low as 1 × 10 −9 A cm −2 at 80 K, 11 × 10 −3 A cm −2 at 150 K, which is comparable to the state-of-the-art PIN superlattice photodetectors with a similar cutoff wavelength [25][26][27]. One can observe a quick increase of dark current density with the bias from 0 to −0.25 V at 80 K. As the temperature increases above 100 K, the dark current densities change little with negative bias indicating that the diffusion dark current dominates.…”
Section: E E I I E Lmentioning
confidence: 55%
“…Figure 5 shows the current-voltage curves of the ICIP-2 at different temperatures. The dark current density at −0.05 V is as low as 1 × 10 −9 A cm −2 at 80 K, 11 × 10 −3 A cm −2 at 150 K, which is comparable to the state-of-the-art PIN superlattice photodetectors with a similar cutoff wavelength [25][26][27]. One can observe a quick increase of dark current density with the bias from 0 to −0.25 V at 80 K. As the temperature increases above 100 K, the dark current densities change little with negative bias indicating that the diffusion dark current dominates.…”
Section: E E I I E Lmentioning
confidence: 55%
“…where QE , N QE DR and QE P are constituents of quantum efficiencies from n, depletion region and p regions, respectively. [19], x , n x p and x DR are the thickness of n, p and depletion regions as calculated in our previous studies [14,20]). The device parameters used in the calculations are listed in table 1.…”
Section: Methodsmentioning
confidence: 99%
“…Since then, various T2SL barrier designs have been extensively developed including nBn, [129,148,168,172,183,191,192] pBn, [146,162] nBp, [87,171,193] pMp, [154,194] niBin, [195] niBn, [164,165] pBiBn, [169,170] and complementary barrier infrared detector (CBIRD). [166,196] Other novel barrier structures include M-structure [176,197,198] (implemented to suppress the tunneling current which leads to an increase in the doping concentration of the active region, and suppression of diffusion current), W-structure [199] (incorporated to suppress tunneling and G-R currents), and N-structure [200][201][202] (employed to improve the wavefunction overlap of spatially separated electrons and holes leading to enhancement in QE). The fundamental principle behind the incorporation of these barrier layers is the confinement of the electric field zone to the wide bandgap barrier material instead of the absorber region so that the SRH process occurs in the barrier and not in the absorber region.…”
Section: Dark Current Densitymentioning
confidence: 99%