The minority carrier lifetime in doped and undoped p-type Hg0.78Cd0.22Te liquid phase epitaxy films |
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Authors: | M C Chen L Colombo J A Dodge J H Tregilgas |
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Affiliation: | (1) Texas Instruments Incorporated, Corporate Research and Development, 75265 Dallas, TX |
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Abstract: | This paper will describe: (1) the first comparative study of recombination mechanisms between doped and undoped p-type Hg1-xCdxTe liquid phase epitaxy films with an x value of about 0.22, and (2) the first determination of τA7
i/τA1
i ratio by lifetime’s dependence on both carrier concentration and temperature. The doped films were either copper- or gold-doped
with the carrier concentration ranging from 2 x 1015 to 1.5 x 1017 cm-3, and the lifetime varied from 2 μs to 8 ns. The undoped (Hg-vacancy) films had a carrier concentration range between 3 x
1015 and 8 x 1016 cm-3, and the lifetime changed from 150 to 3 ns. It was found that for the same carrier concentration, the doped films had lifetimes
several times longer than those of the undoped films, limited mostly by Auger 7 and radiative recombination processes. The
ineffectiveness of Shockley-Read-Hall (SRH) recombination process in the doped films was also demonstrated in lifetime vs
temperature curves. The important ratio of intrinsic Auger 7 lifetime to intrinsic Auger 1 lifetime, τA7
i/τA1
i, was determined to be about 20 from fitting both concentration and temperature curves. The reduction of minority carrier
lifetime in undoped films can be explained by an effective SRH recombination center associated with the Hg vacancy. Indeed,
a donor-like SRH recombination center located at midgap (Ev+60 meV) with a capture cross section for minority carriers much larger than that for majority carriers was deduced from fitting
lifetime vs temperature curves of undoped films. |
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Keywords: | HgCdTe Impurity doped Minority carrier lifetime Photoconductivity decay |
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