The detection of terahertz waves by semimetallic and by semiconducting materials

We present a survey of photoresponse (PR) measurements of various devices containing quantum wells (QWs) of HgTe of various widths d QW and of InSb. By varying d QW for HgTe, the material properties of the QW material change from semiconducting to semimetallic as d QW is increased above a value of a...

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Veröffentlicht in:Journal of applied physics 2011-01, Vol.109 (1), p.013106-013106-5
Hauptverfasser: Gouider, F., Nachtwei, G., Brüne, C., Buhmann, H., Vasilyev, Yu B., Salman, M., Könemann, J., Buckle, P. D.
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Sprache:eng
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Zusammenfassung:We present a survey of photoresponse (PR) measurements of various devices containing quantum wells (QWs) of HgTe of various widths d QW and of InSb. By varying d QW for HgTe, the material properties of the QW material change from semiconducting to semimetallic as d QW is increased above a value of about 6nm. We have studied the PR of devices made from Cd x Hg 1 − x Te / HgTe / Cd x Hg 1 − x Te wafers with values of the QW width in the range of 6   nm ≤ d QW ≤ 21   nm . Only for samples with semimetallic HgTe QWs, a measurable PR could be detected. However, our investigations of samples made from Al x In 1 − x Sb / InSb / Al x In 1 − x Sb wafers gave evidence that a measurable PR also can appear from devices with a semiconducting QW. Both cyclotron-resonant (CR) and nonresonant (bolometric, BO) interaction mechanisms can contribute to the PR signal. Whereas the CR contribution is dominant in Al x In 1 − x Sb / InSb / Al x In 1 − x Sb samples, in Cd x Hg 1 − x Te / HgTe / Cd x Hg 1 − x Te samples the behavior is more complex. In a sample with d QW = 8   nm , the PR is clearly dominated by the BO contribution. In the PR of another sample of d QW = 12   nm , both contributions (BO and CR) are present. The sample of d QW = 21   nm shows a PR with not clearly separable BO and CR contributions.
ISSN:0021-8979
1089-7550
DOI:10.1063/1.3530727