ELECTRONIC DEVICES
Semiconductor apparatus comprises a split-gate semiconductor device (1) whid has a first layer (3) of a first undoped semiconductor material (e.g. GaAs) and a second layer (4) of a second semiconductor material (e.g. AlGaAs) which is doped through at least part of its thickness. The second material...
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creator | KELLY MICHAEL J WHARAM DAVID A SMITH CHARLES G PEPPER MICAHEL BROWN ROBERT J |
description | Semiconductor apparatus comprises a split-gate semiconductor device (1) whid has a first layer (3) of a first undoped semiconductor material (e.g. GaAs) and a second layer (4) of a second semiconductor material (e.g. AlGaAs) which is doped through at least part of its thickness. The second material has a higher energy band gap than the first material, and the layer form a heterojunction so that electrons from the second layers collect in the first layer to form a two-dimensional electron gas. Drain and source contacts (7,6) are provided on the second layers, and a gate electrode (8) is so configured that on application of a sufficiently large negative bias to the gate electrode a constriction is formed in the first layer through which only a one-dimensional electron gas can pass between the source and drain contacts. The apparatus also includes a bias suply (17) for applying a bias voltage between the source and drain contacts. The source/drain bias is made equal to or greater than Ef/e where Ef is the Fermi energy of electrons in the two-dimensional gas and e is the electron charge. As a result of the large source drain bias, the device exhibits negative resistance, and the apparatus can be used as an oscillator or a detector, operating in the THz range. |
format | Patent |
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The second material has a higher energy band gap than the first material, and the layer form a heterojunction so that electrons from the second layers collect in the first layer to form a two-dimensional electron gas. Drain and source contacts (7,6) are provided on the second layers, and a gate electrode (8) is so configured that on application of a sufficiently large negative bias to the gate electrode a constriction is formed in the first layer through which only a one-dimensional electron gas can pass between the source and drain contacts. The apparatus also includes a bias suply (17) for applying a bias voltage between the source and drain contacts. The source/drain bias is made equal to or greater than Ef/e where Ef is the Fermi energy of electrons in the two-dimensional gas and e is the electron charge. As a result of the large source drain bias, the device exhibits negative resistance, and the apparatus can be used as an oscillator or a detector, operating in the THz range.</description><language>eng</language><subject>BASIC ELECTRIC ELEMENTS ; ELECTRIC SOLID STATE DEVICES NOT OTHERWISE PROVIDED FOR ; ELECTRICITY ; SEMICONDUCTOR DEVICES</subject><creationdate>1992</creationdate><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://worldwide.espacenet.com/publicationDetails/biblio?FT=D&date=19920114&DB=EPODOC&CC=US&NR=5081512A$$EHTML$$P50$$Gepo$$Hfree_for_read</linktohtml><link.rule.ids>230,308,780,885,25564,76547</link.rule.ids><linktorsrc>$$Uhttps://worldwide.espacenet.com/publicationDetails/biblio?FT=D&date=19920114&DB=EPODOC&CC=US&NR=5081512A$$EView_record_in_European_Patent_Office$$FView_record_in_$$GEuropean_Patent_Office$$Hfree_for_read</linktorsrc></links><search><creatorcontrib>KELLY; MICHAEL J</creatorcontrib><creatorcontrib>WHARAM; DAVID A</creatorcontrib><creatorcontrib>SMITH; CHARLES G</creatorcontrib><creatorcontrib>PEPPER; MICAHEL</creatorcontrib><creatorcontrib>BROWN; ROBERT J</creatorcontrib><title>ELECTRONIC DEVICES</title><description>Semiconductor apparatus comprises a split-gate semiconductor device (1) whid has a first layer (3) of a first undoped semiconductor material (e.g. GaAs) and a second layer (4) of a second semiconductor material (e.g. AlGaAs) which is doped through at least part of its thickness. The second material has a higher energy band gap than the first material, and the layer form a heterojunction so that electrons from the second layers collect in the first layer to form a two-dimensional electron gas. Drain and source contacts (7,6) are provided on the second layers, and a gate electrode (8) is so configured that on application of a sufficiently large negative bias to the gate electrode a constriction is formed in the first layer through which only a one-dimensional electron gas can pass between the source and drain contacts. The apparatus also includes a bias suply (17) for applying a bias voltage between the source and drain contacts. The source/drain bias is made equal to or greater than Ef/e where Ef is the Fermi energy of electrons in the two-dimensional gas and e is the electron charge. As a result of the large source drain bias, the device exhibits negative resistance, and the apparatus can be used as an oscillator or a detector, operating in the THz range.</description><subject>BASIC ELECTRIC ELEMENTS</subject><subject>ELECTRIC SOLID STATE DEVICES NOT OTHERWISE PROVIDED FOR</subject><subject>ELECTRICITY</subject><subject>SEMICONDUCTOR DEVICES</subject><fulltext>true</fulltext><rsrctype>patent</rsrctype><creationdate>1992</creationdate><recordtype>patent</recordtype><sourceid>EVB</sourceid><recordid>eNrjZBBy9XF1Dgny9_N0VnBxDfN0dg3mYWBNS8wpTuWF0twM8m6uIc4euqkF-fGpxQWJyal5qSXxocGmBhaGpoZGjsaEVQAAzjEdWg</recordid><startdate>19920114</startdate><enddate>19920114</enddate><creator>KELLY; MICHAEL J</creator><creator>WHARAM; DAVID A</creator><creator>SMITH; CHARLES G</creator><creator>PEPPER; MICAHEL</creator><creator>BROWN; ROBERT J</creator><scope>EVB</scope></search><sort><creationdate>19920114</creationdate><title>ELECTRONIC DEVICES</title><author>KELLY; MICHAEL J ; WHARAM; DAVID A ; SMITH; CHARLES G ; PEPPER; MICAHEL ; BROWN; ROBERT J</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-epo_espacenet_US5081512A3</frbrgroupid><rsrctype>patents</rsrctype><prefilter>patents</prefilter><language>eng</language><creationdate>1992</creationdate><topic>BASIC ELECTRIC ELEMENTS</topic><topic>ELECTRIC SOLID STATE DEVICES NOT OTHERWISE PROVIDED FOR</topic><topic>ELECTRICITY</topic><topic>SEMICONDUCTOR DEVICES</topic><toplevel>online_resources</toplevel><creatorcontrib>KELLY; MICHAEL J</creatorcontrib><creatorcontrib>WHARAM; DAVID A</creatorcontrib><creatorcontrib>SMITH; CHARLES G</creatorcontrib><creatorcontrib>PEPPER; MICAHEL</creatorcontrib><creatorcontrib>BROWN; ROBERT J</creatorcontrib><collection>esp@cenet</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>KELLY; MICHAEL J</au><au>WHARAM; DAVID A</au><au>SMITH; CHARLES G</au><au>PEPPER; MICAHEL</au><au>BROWN; ROBERT J</au><format>patent</format><genre>patent</genre><ristype>GEN</ristype><title>ELECTRONIC DEVICES</title><date>1992-01-14</date><risdate>1992</risdate><abstract>Semiconductor apparatus comprises a split-gate semiconductor device (1) whid has a first layer (3) of a first undoped semiconductor material (e.g. GaAs) and a second layer (4) of a second semiconductor material (e.g. AlGaAs) which is doped through at least part of its thickness. The second material has a higher energy band gap than the first material, and the layer form a heterojunction so that electrons from the second layers collect in the first layer to form a two-dimensional electron gas. Drain and source contacts (7,6) are provided on the second layers, and a gate electrode (8) is so configured that on application of a sufficiently large negative bias to the gate electrode a constriction is formed in the first layer through which only a one-dimensional electron gas can pass between the source and drain contacts. The apparatus also includes a bias suply (17) for applying a bias voltage between the source and drain contacts. The source/drain bias is made equal to or greater than Ef/e where Ef is the Fermi energy of electrons in the two-dimensional gas and e is the electron charge. As a result of the large source drain bias, the device exhibits negative resistance, and the apparatus can be used as an oscillator or a detector, operating in the THz range.</abstract><oa>free_for_read</oa></addata></record> |
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subjects | BASIC ELECTRIC ELEMENTS ELECTRIC SOLID STATE DEVICES NOT OTHERWISE PROVIDED FOR ELECTRICITY SEMICONDUCTOR DEVICES |
title | ELECTRONIC DEVICES |
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