Negative luminescence from large-area HgCdTe photodiode arrays with 4.8-6.0-/spl mu/m cutoff wavelengths

We demonstrate the substantial suppression of infrared (IR) blackbody emission from HgCdTe photodiode arrays with cutoff wavelengths of 4.8, 5.5, and 6.0 /spl mu/m. At room temperature, a reverse bias induces internal negative luminescence (NL) efficiencies of 95%, 93%, and 88%, respectively, which...

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Veröffentlicht in:IEEE journal of quantum electronics 2005-02, Vol.41 (2), p.227-233
Hauptverfasser: Lindle, J.R., Bewley, W.W., Vurgaftman, I., Chul Soo Kim, Meyer, J.R., Johnson, J.L., Thomas, M.L., Piquette, E.C., Tennant, W.E.
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container_end_page 233
container_issue 2
container_start_page 227
container_title IEEE journal of quantum electronics
container_volume 41
creator Lindle, J.R.
Bewley, W.W.
Vurgaftman, I.
Chul Soo Kim
Meyer, J.R.
Johnson, J.L.
Thomas, M.L.
Piquette, E.C.
Tennant, W.E.
description We demonstrate the substantial suppression of infrared (IR) blackbody emission from HgCdTe photodiode arrays with cutoff wavelengths of 4.8, 5.5, and 6.0 /spl mu/m. At room temperature, a reverse bias induces internal negative luminescence (NL) efficiencies of 95%, 93%, and 88%, respectively, which correspond to apparent cooling of the surface temperatures by 60, 59, and 49 K. Reverse-bias saturation current densities for the three devices were 0.11, 0.7, and 32 A/cm/sup 2/. Measurement and analysis of the material transmission characteristics indicate that the small residual inefficiencies may be limited by a parasitic absorption process. The 4.8 and 5.5 /spl mu/m photodiodes were fabricated into 18 /spl times/ 2 arrays with total areas of 5 mm /spl times/ 5 mm. In both cases, all 36 array elements were fully operable, and had similar electrical and NL properties. Effective fill factors were /spl ap/100%, since carrier diffusion led to the extraction of carriers from regions between the elements. These results show that efficient, low-power NL devices with active areas in the square-inch range are now feasible for such applications as the cold shielding of infrared focal-plane arrays.
doi_str_mv 10.1109/JQE.2004.839721
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At room temperature, a reverse bias induces internal negative luminescence (NL) efficiencies of 95%, 93%, and 88%, respectively, which correspond to apparent cooling of the surface temperatures by 60, 59, and 49 K. Reverse-bias saturation current densities for the three devices were 0.11, 0.7, and 32 A/cm/sup 2/. Measurement and analysis of the material transmission characteristics indicate that the small residual inefficiencies may be limited by a parasitic absorption process. The 4.8 and 5.5 /spl mu/m photodiodes were fabricated into 18 /spl times/ 2 arrays with total areas of 5 mm /spl times/ 5 mm. In both cases, all 36 array elements were fully operable, and had similar electrical and NL properties. Effective fill factors were /spl ap/100%, since carrier diffusion led to the extraction of carriers from regions between the elements. 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At room temperature, a reverse bias induces internal negative luminescence (NL) efficiencies of 95%, 93%, and 88%, respectively, which correspond to apparent cooling of the surface temperatures by 60, 59, and 49 K. Reverse-bias saturation current densities for the three devices were 0.11, 0.7, and 32 A/cm/sup 2/. Measurement and analysis of the material transmission characteristics indicate that the small residual inefficiencies may be limited by a parasitic absorption process. The 4.8 and 5.5 /spl mu/m photodiodes were fabricated into 18 /spl times/ 2 arrays with total areas of 5 mm /spl times/ 5 mm. In both cases, all 36 array elements were fully operable, and had similar electrical and NL properties. Effective fill factors were /spl ap/100%, since carrier diffusion led to the extraction of carriers from regions between the elements. These results show that efficient, low-power NL devices with active areas in the square-inch range are now feasible for such applications as the cold shielding of infrared focal-plane arrays.</abstract><pub>IEEE</pub><doi>10.1109/JQE.2004.839721</doi><tpages>7</tpages></addata></record>
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subjects Absorption
Charge carrier processes
Cooling
Current density
Infrared (IR) light-emitting diode
Light emitting diodes
Luminescence
midwave IR photodiode
negative luminescence (NL)
Photodiodes
Semiconductor diodes
Temperature
title Negative luminescence from large-area HgCdTe photodiode arrays with 4.8-6.0-/spl mu/m cutoff wavelengths
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