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Linear microwave amplification with Gunn oscillators
Linear microwave amplifiers with continuous power outputs of 100 mW have been constructed utilizing the frequency-independent negative conductance observed externally in Gunn oscillators. This negative conductance is exhibited only in samples containing propagating dipole layers, in other words, n_{...
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Published in: | IEEE transactions on electron devices 1967-09, Vol.14 (9), p.517-522 |
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creator | Thim, H.W. |
description | Linear microwave amplifiers with continuous power outputs of 100 mW have been constructed utilizing the frequency-independent negative conductance observed externally in Gunn oscillators. This negative conductance is exhibited only in samples containing propagating dipole layers, in other words, n_{0} . L must be larger than 10 12 cm -2 for n-GaAs. The output power obtainable from this amplifier is substantially larger than that from a subcritically doped GaAs amplifier ( n_{0} . L < 10^{12} cm -2 ) because n_{0} . L can be increased. Power output and efficiency are discussed in terms of n 0 and L . The upper-frequency limit for amplification is determined by the time the domain takes to readjust itself after a change of external voltage which leads to an upper limit for the f. L product (about 10 8 cm/s). The essential feature of the amplifier circuit is to provide both a short circuit at the Gunn oscillation frequency and a broadband circuit at the signal frequency. An average gain of 3 dB was exhibited from 5.5 GHz to 6.5 GHz. Gain compression of 1 dB occurred at 60 mW output power with 9 dB gain, while the noise figure was about 19 dB. |
doi_str_mv | 10.1109/T-ED.1967.15997 |
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This negative conductance is exhibited only in samples containing propagating dipole layers, in other words, n_{0} . L must be larger than 10 12 cm -2 for n-GaAs. The output power obtainable from this amplifier is substantially larger than that from a subcritically doped GaAs amplifier ( n_{0} . L < 10^{12} cm -2 ) because n_{0} . L can be increased. Power output and efficiency are discussed in terms of n 0 and L . The upper-frequency limit for amplification is determined by the time the domain takes to readjust itself after a change of external voltage which leads to an upper limit for the f. L product (about 10 8 cm/s). The essential feature of the amplifier circuit is to provide both a short circuit at the Gunn oscillation frequency and a broadband circuit at the signal frequency. An average gain of 3 dB was exhibited from 5.5 GHz to 6.5 GHz. Gain compression of 1 dB occurred at 60 mW output power with 9 dB gain, while the noise figure was about 19 dB.</description><identifier>ISSN: 0018-9383</identifier><identifier>EISSN: 1557-9646</identifier><identifier>DOI: 10.1109/T-ED.1967.15997</identifier><identifier>CODEN: IETDAI</identifier><language>eng</language><publisher>IEEE</publisher><ispartof>IEEE transactions on electron devices, 1967-09, Vol.14 (9), p.517-522</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c261t-5f7b202e55efa35edb59510e1670c0af8c2445bf057feac495c8ac68b6d29b3e3</citedby></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/1474720$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>314,780,784,27924,27925,54796</link.rule.ids></links><search><creatorcontrib>Thim, H.W.</creatorcontrib><title>Linear microwave amplification with Gunn oscillators</title><title>IEEE transactions on electron devices</title><addtitle>TED</addtitle><description>Linear microwave amplifiers with continuous power outputs of 100 mW have been constructed utilizing the frequency-independent negative conductance observed externally in Gunn oscillators. This negative conductance is exhibited only in samples containing propagating dipole layers, in other words, n_{0} . L must be larger than 10 12 cm -2 for n-GaAs. The output power obtainable from this amplifier is substantially larger than that from a subcritically doped GaAs amplifier ( n_{0} . L < 10^{12} cm -2 ) because n_{0} . L can be increased. Power output and efficiency are discussed in terms of n 0 and L . The upper-frequency limit for amplification is determined by the time the domain takes to readjust itself after a change of external voltage which leads to an upper limit for the f. L product (about 10 8 cm/s). The essential feature of the amplifier circuit is to provide both a short circuit at the Gunn oscillation frequency and a broadband circuit at the signal frequency. An average gain of 3 dB was exhibited from 5.5 GHz to 6.5 GHz. Gain compression of 1 dB occurred at 60 mW output power with 9 dB gain, while the noise figure was about 19 dB.</description><issn>0018-9383</issn><issn>1557-9646</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1967</creationdate><recordtype>article</recordtype><recordid>eNpFj01LxDAYhIMoWFfPHrz0D6Sb7zRH2a2rUPBSzyHNvsFIP5amuvjv7bqCp2FgZpgHoXtKCkqJWTe42hbUKF1QaYy-QBmVUmOjhLpEGSG0xIaX_BrdpPSxWCUEy5Co4wBuyvvop_HoviB3_aGLIXo3x3HIj3F-z3efw5CPyceuc_M4pVt0FVyX4O5PV-jtqWo2z7h-3b1sHmvsmaIzlkG3jDCQEoLjEvatNJISoEoTT1woPRNCtoFIHcB5YaQvnVdlq_bMtBz4Cq3Pu8u3lCYI9jDF3k3flhJ7graNrbb2BG1_oZfGw7kRAeA_LbTQjPAfEq9Tuw</recordid><startdate>196709</startdate><enddate>196709</enddate><creator>Thim, H.W.</creator><general>IEEE</general><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>196709</creationdate><title>Linear microwave amplification with Gunn oscillators</title><author>Thim, H.W.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c261t-5f7b202e55efa35edb59510e1670c0af8c2445bf057feac495c8ac68b6d29b3e3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1967</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Thim, H.W.</creatorcontrib><collection>CrossRef</collection><jtitle>IEEE transactions on electron devices</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Thim, H.W.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Linear microwave amplification with Gunn oscillators</atitle><jtitle>IEEE transactions on electron devices</jtitle><stitle>TED</stitle><date>1967-09</date><risdate>1967</risdate><volume>14</volume><issue>9</issue><spage>517</spage><epage>522</epage><pages>517-522</pages><issn>0018-9383</issn><eissn>1557-9646</eissn><coden>IETDAI</coden><abstract>Linear microwave amplifiers with continuous power outputs of 100 mW have been constructed utilizing the frequency-independent negative conductance observed externally in Gunn oscillators. This negative conductance is exhibited only in samples containing propagating dipole layers, in other words, n_{0} . L must be larger than 10 12 cm -2 for n-GaAs. The output power obtainable from this amplifier is substantially larger than that from a subcritically doped GaAs amplifier ( n_{0} . L < 10^{12} cm -2 ) because n_{0} . L can be increased. Power output and efficiency are discussed in terms of n 0 and L . The upper-frequency limit for amplification is determined by the time the domain takes to readjust itself after a change of external voltage which leads to an upper limit for the f. L product (about 10 8 cm/s). The essential feature of the amplifier circuit is to provide both a short circuit at the Gunn oscillation frequency and a broadband circuit at the signal frequency. An average gain of 3 dB was exhibited from 5.5 GHz to 6.5 GHz. Gain compression of 1 dB occurred at 60 mW output power with 9 dB gain, while the noise figure was about 19 dB.</abstract><pub>IEEE</pub><doi>10.1109/T-ED.1967.15997</doi><tpages>6</tpages></addata></record> |
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title | Linear microwave amplification with Gunn oscillators |
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