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InAs/(GaIn)Sb short-period superlattices for focal plane arrays

InAs/(GaIn)Sb short-period superlattices for focal plane arrays

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on the mesa sidewalls. Some larger diodes show significantly higher (R0A) -1 values which are attributed to growth<br />

defects in the bulk of the diode. This interpretation is in accordance with the histogram of 12 quadratic diodes with 70<br />

µm edge length (P/A = 0.057 µm -1 ) from Figure 10a, which is shown in Figure 10b. Only one diode (#11) out of 12<br />

randomly selected diodes differs significantly from R0A ≈ 5 – 10 Ωcm 2 . Further experimental investigations, which are<br />

beyond the scope of this paper, do not suggest any problems with the long-term stability or reproducibility of the<br />

Al0.5Ga0.5As0.04<strong>Sb</strong>0.96 passivation.<br />

4. CONCLUSIONS<br />

Important progress on <strong>short</strong>-<strong>period</strong> p-i-n superlattice photodiodes based on the <strong>InAs</strong>/<strong>GaIn</strong><strong>Sb</strong> material system could be<br />

achieved in both atmospheric transmission windows in the infrared spectral range. In the 3-5 µm regime the first fully<br />

operational 256x256 camera system was demonstrated exhibiting a NETD per<strong>for</strong>mance of 9.4 mK at 6.5 ms integration<br />

time with F/2 optics at 73 K. The excellent homogeneity of the electro-optical per<strong>for</strong>mance combined with the very low<br />

pixel outages without any large cluster defects constitute an important advantage over state-of-the-art HgCdTe detectors<br />

at comparable per<strong>for</strong>mance. In the 8-10 µm region a method based on the epitaxial MBE overgrowth with high bandgap<br />

AlGaAs<strong>Sb</strong> offers a stable method to passivate <strong>InAs</strong>/<strong>GaIn</strong><strong>Sb</strong> superlattice photodiodes. No surface leakage currents were<br />

observed in test diodes as small as 70 µm diameter. Since the illustrated approach is compatible with standard device<br />

processing, the realization of the first superlattice FPA in the 8-10 µm window seems within reach.<br />

ACKOWLEDGMENTS<br />

The authors are grateful to K. Schwarz, H. Güllich, L. Kirste and K. Windscheid <strong>for</strong> characterization of detector<br />

structures. We also express our thanks to P. Koidl and G. Weimann <strong>for</strong> fruitful discussions. Financing support by the<br />

Federal Ministry of Defense is gratefully acknowledged.<br />

REFERENCES<br />

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