Mercury Cadmium Telluride 2010
DOI: 10.1002/9780470669464.ch4
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Substrates for the Epitaxial Growth of MCT

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Cited by 4 publications
(8 citation statements)
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“…Note that the high density of dislocation‐related states shown in Figure S2, Supporting Information is due to the high simulated dislocation areal density of ≈2.9 × 10 13 cm −2 for the 192‐atom supercell and ≈1.3 × 10 13 cm −2 for the 432‐atom supercell. This is in contrast to practical device‐grade materials that have much lower dislocation densities ranging from ≈10 4 cm −2 for higher quality materials to ≈10 6 cm −2 for lower quality materials, [ 5 ] and thus have a much lower density of dislocation‐related states within the energy bandgap. Nevertheless, these simulations allow us to observe the energy positions of the trap states that these dislocations introduce within the bandgap.…”
Section: Resultsmentioning
confidence: 88%
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“…Note that the high density of dislocation‐related states shown in Figure S2, Supporting Information is due to the high simulated dislocation areal density of ≈2.9 × 10 13 cm −2 for the 192‐atom supercell and ≈1.3 × 10 13 cm −2 for the 432‐atom supercell. This is in contrast to practical device‐grade materials that have much lower dislocation densities ranging from ≈10 4 cm −2 for higher quality materials to ≈10 6 cm −2 for lower quality materials, [ 5 ] and thus have a much lower density of dislocation‐related states within the energy bandgap. Nevertheless, these simulations allow us to observe the energy positions of the trap states that these dislocations introduce within the bandgap.…”
Section: Resultsmentioning
confidence: 88%
“…This may be a possible explanation for the enhanced interdiffusion of HgTe/CdTe superlattices in regions around dislocations. [ 5 ]…”
Section: Resultsmentioning
confidence: 99%
“…While the lattice matching of CZT substrates reduces the formation of misfit dislocations, commercially available CZT substrates often have a high density of surface dislocations (∼10 4 cm −2 ), which thread into the MCT epilayer during MBE growth. 3 Threading dislocations are undesirable if they intersect the depletion region (the exact position in the epilayer depends on the specific device structure) of MCT detectors as they act as sources of tunnel current and 1/f noise, which limits the performance of these detectors. 4 Thus, a better understanding of how dislocations thread from the substrate to the epilayer during the growth process would assist in narrowing down the dominant types of dislocations that may be present in the MCT epilayer.…”
Section: ■ Introductionmentioning
confidence: 99%
“…The production of high crystalline quality MCT is achieved by molecular beam epitaxy (MBE) growth on lattice-matched Cd 0.96 Zn 0.04 Te (CZT) substrates of a (211)B orientation. While the lattice matching of CZT substrates reduces the formation of misfit dislocations, commercially available CZT substrates often have a high density of surface dislocations (∼10 4 cm –2 ), which thread into the MCT epilayer during MBE growth . Threading dislocations are undesirable if they intersect the depletion region (the exact position in the epilayer depends on the specific device structure) of MCT detectors as they act as sources of tunnel current and 1/ f noise, which limits the performance of these detectors .…”
Section: Introductionmentioning
confidence: 99%
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