Comparison of unit cell coupling for grating‐gate and high electron mobilitytransistor array THz resonant absorbers
We report experimental studies on the excitation of synchronized plasmon resonances inAlGaN/GaN High Electron Mobility Transistor (HEMT) arrays. In contrast to the commonlyemployed grating-gate configurations, the analyzed structure contains periodicallypatterned ohmic contacts to the two-dimensiona...
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Veröffentlicht in: | Journal of applied physics 2018-09, Vol.124 (9) |
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creator | Condori Quispe Hugo O Chanana Ashish Encomendero Jimy Zhu Mingda Trometer Nicole Nahata Ajay Jena Debdeep Xing Huili Grace Sensale-Rodriguez Berardi |
description | We report experimental studies on the excitation of synchronized plasmon resonances inAlGaN/GaN High Electron Mobility Transistor (HEMT) arrays. In contrast to the commonlyemployed grating-gate configurations, the analyzed structure contains periodicallypatterned ohmic contacts to the two-dimensional electron gas, which are laid-out parallelto the gate fingers. In this structure, the terahertz to plasmon coupling mechanism isfundamentally different from that in grating-gate configurations. Whereas the grating-gateconfiguration constitutes a coupled resonant system in whichthe resonance frequency depends on the grating periodicity, when periodical ohmic contactsare incorporated, the system behaves as a synchronizedresonant system in which each unit cell is effectively independent. As a result, in aHEMT-array, the resonance is no longer set by the periodicity but rather by the gate andthe ungated region length. Experimental results of fabricated samples compare well withnumerical simulations and theoretical expectations. Our work demonstrates that theproposed approach allows: (i) more efficient excitation ofhigh order plasmon modes and (ii) superior overall terahertzto plasmon coupling, even in configurations having less number of devices per unit area.From this perspective, our results reveal a simple way to enhance the terahertz to plasmoncoupling and thus improve the performance of electron plasma wave-based devices; thiseffect can be exploited, for example, to improve the response of HEMT-based terahertzdetectors. |
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In contrast to the commonlyemployed grating-gate configurations, the analyzed structure contains periodicallypatterned ohmic contacts to the two-dimensional electron gas, which are laid-out parallelto the gate fingers. In this structure, the terahertz to plasmon coupling mechanism isfundamentally different from that in grating-gate configurations. Whereas the grating-gateconfiguration constitutes a coupled resonant system in whichthe resonance frequency depends on the grating periodicity, when periodical ohmic contactsare incorporated, the system behaves as a synchronizedresonant system in which each unit cell is effectively independent. As a result, in aHEMT-array, the resonance is no longer set by the periodicity but rather by the gate andthe ungated region length. Experimental results of fabricated samples compare well withnumerical simulations and theoretical expectations. Our work demonstrates that theproposed approach allows: (i) more efficient excitation ofhigh order plasmon modes and (ii) superior overall terahertzto plasmon coupling, even in configurations having less number of devices per unit area.From this perspective, our results reveal a simple way to enhance the terahertz to plasmoncoupling and thus improve the performance of electron plasma wave-based devices; thiseffect can be exploited, for example, to improve the response of HEMT-based terahertzdetectors.</description><identifier>ISSN: 0021-8979</identifier><identifier>EISSN: 1089-7550</identifier><language>eng</language><publisher>Melville: American Institute of Physics</publisher><subject>Applied physics ; Arrays ; Configurations ; Contact resistance ; Coupling ; Electron gas ; Electron mobility ; Electron plasma ; Excitation ; Performance enhancement ; Periodic variations ; Plasma waves ; Unit cell</subject><ispartof>Journal of applied physics, 2018-09, Vol.124 (9)</ispartof><rights>2018 Author(s). Published by AIP Publishing.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780</link.rule.ids></links><search><creatorcontrib>Condori Quispe Hugo O</creatorcontrib><creatorcontrib>Chanana Ashish</creatorcontrib><creatorcontrib>Encomendero Jimy</creatorcontrib><creatorcontrib>Zhu Mingda</creatorcontrib><creatorcontrib>Trometer Nicole</creatorcontrib><creatorcontrib>Nahata Ajay</creatorcontrib><creatorcontrib>Jena Debdeep</creatorcontrib><creatorcontrib>Xing Huili Grace</creatorcontrib><creatorcontrib>Sensale-Rodriguez Berardi</creatorcontrib><title>Comparison of unit cell coupling for grating‐gate and high electron mobilitytransistor array THz resonant absorbers</title><title>Journal of applied physics</title><description>We report experimental studies on the excitation of synchronized plasmon resonances inAlGaN/GaN High Electron Mobility Transistor (HEMT) arrays. In contrast to the commonlyemployed grating-gate configurations, the analyzed structure contains periodicallypatterned ohmic contacts to the two-dimensional electron gas, which are laid-out parallelto the gate fingers. In this structure, the terahertz to plasmon coupling mechanism isfundamentally different from that in grating-gate configurations. Whereas the grating-gateconfiguration constitutes a coupled resonant system in whichthe resonance frequency depends on the grating periodicity, when periodical ohmic contactsare incorporated, the system behaves as a synchronizedresonant system in which each unit cell is effectively independent. As a result, in aHEMT-array, the resonance is no longer set by the periodicity but rather by the gate andthe ungated region length. Experimental results of fabricated samples compare well withnumerical simulations and theoretical expectations. Our work demonstrates that theproposed approach allows: (i) more efficient excitation ofhigh order plasmon modes and (ii) superior overall terahertzto plasmon coupling, even in configurations having less number of devices per unit area.From this perspective, our results reveal a simple way to enhance the terahertz to plasmoncoupling and thus improve the performance of electron plasma wave-based devices; thiseffect can be exploited, for example, to improve the response of HEMT-based terahertzdetectors.</description><subject>Applied physics</subject><subject>Arrays</subject><subject>Configurations</subject><subject>Contact resistance</subject><subject>Coupling</subject><subject>Electron gas</subject><subject>Electron mobility</subject><subject>Electron plasma</subject><subject>Excitation</subject><subject>Performance enhancement</subject><subject>Periodic variations</subject><subject>Plasma waves</subject><subject>Unit cell</subject><issn>0021-8979</issn><issn>1089-7550</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2018</creationdate><recordtype>article</recordtype><recordid>eNqNjEFOwzAQRS0EEgF6h5FYR7JbtY3XFagH6L6aBCd15XrSmfGirDgCZ-QkeMEBWP0v_ff-nWmc7Xy7Xa_tvWmsXbq281v_aJ5EztY61618Y8qOLjNyFMpAI5QcFYaQEgxU5hTzBCMxTIxa-8_X94QaAPMHnOJ0gpDCoFzVC_UxRb0pY5YoWh1kxhsc9p_Aob5jVsBeiPvA8mIeRkwSFn_5bF7f3w67fTszXUsQPZ6pcK7TcWm9d37jNm71P-oX7ytQKQ</recordid><startdate>20180907</startdate><enddate>20180907</enddate><creator>Condori Quispe Hugo O</creator><creator>Chanana Ashish</creator><creator>Encomendero Jimy</creator><creator>Zhu Mingda</creator><creator>Trometer Nicole</creator><creator>Nahata Ajay</creator><creator>Jena Debdeep</creator><creator>Xing Huili Grace</creator><creator>Sensale-Rodriguez Berardi</creator><general>American Institute of Physics</general><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope></search><sort><creationdate>20180907</creationdate><title>Comparison of unit cell coupling for grating‐gate and high electron mobilitytransistor array THz resonant absorbers</title><author>Condori Quispe Hugo O ; Chanana Ashish ; Encomendero Jimy ; Zhu Mingda ; Trometer Nicole ; Nahata Ajay ; Jena Debdeep ; Xing Huili Grace ; Sensale-Rodriguez Berardi</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-proquest_journals_20991961613</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2018</creationdate><topic>Applied physics</topic><topic>Arrays</topic><topic>Configurations</topic><topic>Contact resistance</topic><topic>Coupling</topic><topic>Electron gas</topic><topic>Electron mobility</topic><topic>Electron plasma</topic><topic>Excitation</topic><topic>Performance enhancement</topic><topic>Periodic variations</topic><topic>Plasma waves</topic><topic>Unit cell</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Condori Quispe Hugo O</creatorcontrib><creatorcontrib>Chanana Ashish</creatorcontrib><creatorcontrib>Encomendero Jimy</creatorcontrib><creatorcontrib>Zhu Mingda</creatorcontrib><creatorcontrib>Trometer Nicole</creatorcontrib><creatorcontrib>Nahata Ajay</creatorcontrib><creatorcontrib>Jena Debdeep</creatorcontrib><creatorcontrib>Xing Huili Grace</creatorcontrib><creatorcontrib>Sensale-Rodriguez Berardi</creatorcontrib><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of applied physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Condori Quispe Hugo O</au><au>Chanana Ashish</au><au>Encomendero Jimy</au><au>Zhu Mingda</au><au>Trometer Nicole</au><au>Nahata Ajay</au><au>Jena Debdeep</au><au>Xing Huili Grace</au><au>Sensale-Rodriguez Berardi</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Comparison of unit cell coupling for grating‐gate and high electron mobilitytransistor array THz resonant absorbers</atitle><jtitle>Journal of applied physics</jtitle><date>2018-09-07</date><risdate>2018</risdate><volume>124</volume><issue>9</issue><issn>0021-8979</issn><eissn>1089-7550</eissn><abstract>We report experimental studies on the excitation of synchronized plasmon resonances inAlGaN/GaN High Electron Mobility Transistor (HEMT) arrays. In contrast to the commonlyemployed grating-gate configurations, the analyzed structure contains periodicallypatterned ohmic contacts to the two-dimensional electron gas, which are laid-out parallelto the gate fingers. In this structure, the terahertz to plasmon coupling mechanism isfundamentally different from that in grating-gate configurations. Whereas the grating-gateconfiguration constitutes a coupled resonant system in whichthe resonance frequency depends on the grating periodicity, when periodical ohmic contactsare incorporated, the system behaves as a synchronizedresonant system in which each unit cell is effectively independent. As a result, in aHEMT-array, the resonance is no longer set by the periodicity but rather by the gate andthe ungated region length. Experimental results of fabricated samples compare well withnumerical simulations and theoretical expectations. Our work demonstrates that theproposed approach allows: (i) more efficient excitation ofhigh order plasmon modes and (ii) superior overall terahertzto plasmon coupling, even in configurations having less number of devices per unit area.From this perspective, our results reveal a simple way to enhance the terahertz to plasmoncoupling and thus improve the performance of electron plasma wave-based devices; thiseffect can be exploited, for example, to improve the response of HEMT-based terahertzdetectors.</abstract><cop>Melville</cop><pub>American Institute of Physics</pub></addata></record> |
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subjects | Applied physics Arrays Configurations Contact resistance Coupling Electron gas Electron mobility Electron plasma Excitation Performance enhancement Periodic variations Plasma waves Unit cell |
title | Comparison of unit cell coupling for grating‐gate and high electron mobilitytransistor array THz resonant absorbers |
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