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Negative transconductance in monocrystalline (Al,Ga)As/NiAl/(Al,Ga)As semiconductor/metal/semiconductor tunneling transistors
The authors present the three-terminal transport characteristics of a resonant-tunneling semiconductor-metal-semiconductor (SMS) structure. The buried metal quantum well consists of a 3-nm-thick NiAl layer, epitaxially integrated in (Al,Ga)As, and is contacted by selectively removing the semiconduct...
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Published in: | IEEE transactions on electron devices 1989-11, Vol.36 (11), p.2620-2621 |
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container_end_page | 2621 |
container_issue | 11 |
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container_title | IEEE transactions on electron devices |
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creator | Tabatabaie, N. Sands, T. Harbison, J.P. Gilchrist, H.L. Cheeks, T.L. Florez, L.T. Keramidas, V.G. |
description | The authors present the three-terminal transport characteristics of a resonant-tunneling semiconductor-metal-semiconductor (SMS) structure. The buried metal quantum well consists of a 3-nm-thick NiAl layer, epitaxially integrated in (Al,Ga)As, and is contacted by selectively removing the semiconductor overgrowth. The undoped AlAs tunneling barriers are 2 nm thick and are set back by 5 nm of undoped GaAs from the doped GaAs electrodes. The GaAs doping densities were adjusted to allow for the fabrication of emitter-up, collector-up, and symmetric transistors. The metal-semiconductor Schottky contacts between the NiAl and the cladding (Al,Ga)As layers were studied in order to characterize the individual interfaces and also to confirm the independence of the ultrathin buried metal electrode. Transistor action has been observed at room temperature in emitter-up structures with a wide (70 nm) undoped GaAs collector spacer. Room-temperature negative transconductance values as high as 1.4 mS/mm/sup 2/ have been obtained for large-area (80- mu m diameter) devices. |
doi_str_mv | 10.1109/16.43740 |
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The buried metal quantum well consists of a 3-nm-thick NiAl layer, epitaxially integrated in (Al,Ga)As, and is contacted by selectively removing the semiconductor overgrowth. The undoped AlAs tunneling barriers are 2 nm thick and are set back by 5 nm of undoped GaAs from the doped GaAs electrodes. The GaAs doping densities were adjusted to allow for the fabrication of emitter-up, collector-up, and symmetric transistors. The metal-semiconductor Schottky contacts between the NiAl and the cladding (Al,Ga)As layers were studied in order to characterize the individual interfaces and also to confirm the independence of the ultrathin buried metal electrode. Transistor action has been observed at room temperature in emitter-up structures with a wide (70 nm) undoped GaAs collector spacer. 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The buried metal quantum well consists of a 3-nm-thick NiAl layer, epitaxially integrated in (Al,Ga)As, and is contacted by selectively removing the semiconductor overgrowth. The undoped AlAs tunneling barriers are 2 nm thick and are set back by 5 nm of undoped GaAs from the doped GaAs electrodes. The GaAs doping densities were adjusted to allow for the fabrication of emitter-up, collector-up, and symmetric transistors. The metal-semiconductor Schottky contacts between the NiAl and the cladding (Al,Ga)As layers were studied in order to characterize the individual interfaces and also to confirm the independence of the ultrathin buried metal electrode. Transistor action has been observed at room temperature in emitter-up structures with a wide (70 nm) undoped GaAs collector spacer. Room-temperature negative transconductance values as high as 1.4 mS/mm/sup 2/ have been obtained for large-area (80- mu m diameter) devices.</description><subject>Electrodes</subject><subject>Fabrication</subject><subject>Gallium arsenide</subject><subject>Resonant tunneling devices</subject><subject>Schottky barriers</subject><subject>Semiconductor device doping</subject><subject>Temperature</subject><subject>Transconductance</subject><issn>0018-9383</issn><issn>1557-9646</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1989</creationdate><recordtype>article</recordtype><recordid>eNqNkc1Lw0AQxRdRsFbBq7ecpIJpdrOb_TiGolUo9aLnsG4mZSXZ1N1E6MH_3WhKwVtPw3vzezOHh9A1wXNCsEoInzMqGD5BE5JlIlac8VM0wZjIWFFJz9FFCB-D5IylE_S9ho3u7BdEndcumNaVvem0MxBZFzWta43fhU7XtXUQzfL6fqnv8pCsbV4nBxkFaOw-2_qkgSGQ_POirncOhiOb8ZENgxku0Vml6wBX-zlFb48Pr4unePWyfF7kq9gQxlQsFC-FNEyZKjXYYM4HX0ml3nkqKM0wxUpmXBBIoTRclhmnohI65aAYAUOn6Ha8u_XtZw-hKxobDNS1dtD2oUilypRQ6ghQYiyZPAJklBKZDuBsBI1vQ_BQFVtvG-13BcHFb2MF4cVfYwN6M6IWAA7YuPsBIDKQvQ</recordid><startdate>198911</startdate><enddate>198911</enddate><creator>Tabatabaie, N.</creator><creator>Sands, T.</creator><creator>Harbison, J.P.</creator><creator>Gilchrist, H.L.</creator><creator>Cheeks, T.L.</creator><creator>Florez, L.T.</creator><creator>Keramidas, V.G.</creator><general>IEEE</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>8FD</scope><scope>L7M</scope><scope>7QF</scope><scope>8BQ</scope><scope>JG9</scope><scope>7U5</scope></search><sort><creationdate>198911</creationdate><title>Negative transconductance in monocrystalline (Al,Ga)As/NiAl/(Al,Ga)As semiconductor/metal/semiconductor tunneling transistors</title><author>Tabatabaie, N. ; Sands, T. ; Harbison, J.P. ; Gilchrist, H.L. ; Cheeks, T.L. ; Florez, L.T. ; Keramidas, V.G.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c1449-796d78c49cf2c0c066c149899b627335030985671e2edc68d5637f7a26e941ec3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1989</creationdate><topic>Electrodes</topic><topic>Fabrication</topic><topic>Gallium arsenide</topic><topic>Resonant tunneling devices</topic><topic>Schottky barriers</topic><topic>Semiconductor device doping</topic><topic>Temperature</topic><topic>Transconductance</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Tabatabaie, N.</creatorcontrib><creatorcontrib>Sands, T.</creatorcontrib><creatorcontrib>Harbison, J.P.</creatorcontrib><creatorcontrib>Gilchrist, H.L.</creatorcontrib><creatorcontrib>Cheeks, T.L.</creatorcontrib><creatorcontrib>Florez, L.T.</creatorcontrib><creatorcontrib>Keramidas, V.G.</creatorcontrib><collection>CrossRef</collection><collection>Electronics & Communications Abstracts</collection><collection>Technology Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Aluminium Industry Abstracts</collection><collection>METADEX</collection><collection>Materials Research Database</collection><collection>Solid State and Superconductivity Abstracts</collection><jtitle>IEEE transactions on electron devices</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Tabatabaie, N.</au><au>Sands, T.</au><au>Harbison, J.P.</au><au>Gilchrist, H.L.</au><au>Cheeks, T.L.</au><au>Florez, L.T.</au><au>Keramidas, V.G.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Negative transconductance in monocrystalline (Al,Ga)As/NiAl/(Al,Ga)As semiconductor/metal/semiconductor tunneling transistors</atitle><jtitle>IEEE transactions on electron devices</jtitle><stitle>TED</stitle><date>1989-11</date><risdate>1989</risdate><volume>36</volume><issue>11</issue><spage>2620</spage><epage>2621</epage><pages>2620-2621</pages><issn>0018-9383</issn><eissn>1557-9646</eissn><coden>IETDAI</coden><abstract>The authors present the three-terminal transport characteristics of a resonant-tunneling semiconductor-metal-semiconductor (SMS) structure. The buried metal quantum well consists of a 3-nm-thick NiAl layer, epitaxially integrated in (Al,Ga)As, and is contacted by selectively removing the semiconductor overgrowth. The undoped AlAs tunneling barriers are 2 nm thick and are set back by 5 nm of undoped GaAs from the doped GaAs electrodes. The GaAs doping densities were adjusted to allow for the fabrication of emitter-up, collector-up, and symmetric transistors. The metal-semiconductor Schottky contacts between the NiAl and the cladding (Al,Ga)As layers were studied in order to characterize the individual interfaces and also to confirm the independence of the ultrathin buried metal electrode. Transistor action has been observed at room temperature in emitter-up structures with a wide (70 nm) undoped GaAs collector spacer. Room-temperature negative transconductance values as high as 1.4 mS/mm/sup 2/ have been obtained for large-area (80- mu m diameter) devices.</abstract><pub>IEEE</pub><doi>10.1109/16.43740</doi><tpages>2</tpages></addata></record> |
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ispartof | IEEE transactions on electron devices, 1989-11, Vol.36 (11), p.2620-2621 |
issn | 0018-9383 1557-9646 |
language | eng |
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source | IEEE Electronic Library (IEL) Journals |
subjects | Electrodes Fabrication Gallium arsenide Resonant tunneling devices Schottky barriers Semiconductor device doping Temperature Transconductance |
title | Negative transconductance in monocrystalline (Al,Ga)As/NiAl/(Al,Ga)As semiconductor/metal/semiconductor tunneling transistors |
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