A Theoretical Treatment of THz Resonances in Semiconductor GaAs p-n Junctions
Semiconductor heterostructures are suitable for the design and fabrication of terahertz (THz) plasmonic devices, due to their matching carrier densities. The classical dispersion relations in the current literature are derived for metal plasmonic materials, such as gold and silver, for which a homog...
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description | Semiconductor heterostructures are suitable for the design and fabrication of terahertz (THz) plasmonic devices, due to their matching carrier densities. The classical dispersion relations in the current literature are derived for metal plasmonic materials, such as gold and silver, for which a homogeneous dielectric function is valid. Penetration of the electric fields into semiconductors induces locally varying charge densities and a spatially varying dielectric function is expected. While such an occurrence renders tunable THz plasmonics a possibility, it is crucial to understand the conditions under which propagating resonant conditions for the carriers occur, upon incidence of an electromagnetic radiation. In this manuscript, we derive a dispersion relation for a p-n heterojunction and apply the methodology to a GaAs p-n junction, a material of interest for optoelectronic devices. Considering symmetrically doped p- and n-type regions with equal width, the effect of certain parameters (such as doping and voltage bias) on the dispersion curve of the p-n heterojunction were investigated. Keeping in sight the different effective masses and mobilities of the carriers, we were able to obtain the conditions that yield identical dielectric functions for the p- and n-regions. Our results indicated that the p-n GaAs system can sustain propagating resonances and can be used as a layered plasmonic waveguide. The conditions under which this is feasible fall in the frequency region between the transverse optical phonon resonance of GaAs and the traditional cut-off frequency of the diode waveguide. In addition, our results indicated when the excitation was slightly above the phonon resonance frequency, the plasmon propagation attained low-loss characteristics. We also showed that the existence or nonexistence of the depletion zone between the p- and n- interfaces allowed certain plasmon modes to propagate, while others decayed rapidly, pointing out the possibility for a design of selective filters. |
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The classical dispersion relations in the current literature are derived for metal plasmonic materials, such as gold and silver, for which a homogeneous dielectric function is valid. Penetration of the electric fields into semiconductors induces locally varying charge densities and a spatially varying dielectric function is expected. While such an occurrence renders tunable THz plasmonics a possibility, it is crucial to understand the conditions under which propagating resonant conditions for the carriers occur, upon incidence of an electromagnetic radiation. In this manuscript, we derive a dispersion relation for a p-n heterojunction and apply the methodology to a GaAs p-n junction, a material of interest for optoelectronic devices. Considering symmetrically doped p- and n-type regions with equal width, the effect of certain parameters (such as doping and voltage bias) on the dispersion curve of the p-n heterojunction were investigated. Keeping in sight the different effective masses and mobilities of the carriers, we were able to obtain the conditions that yield identical dielectric functions for the p- and n-regions. Our results indicated that the p-n GaAs system can sustain propagating resonances and can be used as a layered plasmonic waveguide. The conditions under which this is feasible fall in the frequency region between the transverse optical phonon resonance of GaAs and the traditional cut-off frequency of the diode waveguide. In addition, our results indicated when the excitation was slightly above the phonon resonance frequency, the plasmon propagation attained low-loss characteristics. We also showed that the existence or nonexistence of the depletion zone between the p- and n- interfaces allowed certain plasmon modes to propagate, while others decayed rapidly, pointing out the possibility for a design of selective filters.</description><identifier>ISSN: 1996-1944</identifier><identifier>EISSN: 1996-1944</identifier><identifier>DOI: 10.3390/ma12152412</identifier><identifier>PMID: 31362342</identifier><language>eng</language><publisher>Switzerland: MDPI AG</publisher><subject>Carrier density ; Current carriers ; Damping ; Doping ; Electric fields ; Electron mass ; Gallium arsenide ; Heterostructures ; Infrared radiation ; Integrated circuits ; Light emitting diodes ; Majority carriers ; Materials selection ; Metals ; Metamaterials ; Modulators ; Multilayers ; Organic light emitting diodes ; P-n junctions ; Photovoltaic cells ; Propagation ; Quantum dots ; Relaxation time ; Semiconductor lasers ; Semiconductors ; Solar cells ; Terahertz frequencies ; Waveguides</subject><ispartof>Materials, 2019-07, Vol.12 (15), p.2412</ispartof><rights>2019. This work is licensed under https://creativecommons.org/licenses/by/4.0/ (the “License”). 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The classical dispersion relations in the current literature are derived for metal plasmonic materials, such as gold and silver, for which a homogeneous dielectric function is valid. Penetration of the electric fields into semiconductors induces locally varying charge densities and a spatially varying dielectric function is expected. While such an occurrence renders tunable THz plasmonics a possibility, it is crucial to understand the conditions under which propagating resonant conditions for the carriers occur, upon incidence of an electromagnetic radiation. In this manuscript, we derive a dispersion relation for a p-n heterojunction and apply the methodology to a GaAs p-n junction, a material of interest for optoelectronic devices. Considering symmetrically doped p- and n-type regions with equal width, the effect of certain parameters (such as doping and voltage bias) on the dispersion curve of the p-n heterojunction were investigated. Keeping in sight the different effective masses and mobilities of the carriers, we were able to obtain the conditions that yield identical dielectric functions for the p- and n-regions. Our results indicated that the p-n GaAs system can sustain propagating resonances and can be used as a layered plasmonic waveguide. The conditions under which this is feasible fall in the frequency region between the transverse optical phonon resonance of GaAs and the traditional cut-off frequency of the diode waveguide. In addition, our results indicated when the excitation was slightly above the phonon resonance frequency, the plasmon propagation attained low-loss characteristics. We also showed that the existence or nonexistence of the depletion zone between the p- and n- interfaces allowed certain plasmon modes to propagate, while others decayed rapidly, pointing out the possibility for a design of selective filters.</description><subject>Carrier density</subject><subject>Current carriers</subject><subject>Damping</subject><subject>Doping</subject><subject>Electric fields</subject><subject>Electron mass</subject><subject>Gallium arsenide</subject><subject>Heterostructures</subject><subject>Infrared radiation</subject><subject>Integrated circuits</subject><subject>Light emitting diodes</subject><subject>Majority carriers</subject><subject>Materials selection</subject><subject>Metals</subject><subject>Metamaterials</subject><subject>Modulators</subject><subject>Multilayers</subject><subject>Organic light emitting diodes</subject><subject>P-n junctions</subject><subject>Photovoltaic cells</subject><subject>Propagation</subject><subject>Quantum dots</subject><subject>Relaxation time</subject><subject>Semiconductor lasers</subject><subject>Semiconductors</subject><subject>Solar cells</subject><subject>Terahertz frequencies</subject><subject>Waveguides</subject><issn>1996-1944</issn><issn>1996-1944</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><recordid>eNpdkU9r3DAQxUVpaMJmL_0ARdBLKTiRNLJsXQrLkr8kBFLfhVYeNw62tJXsQPrpo5BtmmYuMzA_Hm_mEfKZsyMAzY5HywUvheTiAzngWquCayk_vpn3yTKle5YLgNdCfyL7wEEJkOKAXK9oc4ch4tQ7O9Amop1G9BMNHW3O_9BbTMFb7zDR3tOfOPYu-HZ2U4j0zK4S3RaeXs7eTX3w6ZDsdXZIuNz1BWlOT5r1eXF1c3axXl0VTjI1Fa7WWALTineKVW7D5cZJZKyrXSVLsDUX0DFrXQtdWSIq6zRk0qqubesNLMiPF9ntvBmxddlvtIPZxn608dEE25v_N76_M7_Cg1FKl0qUWeDbTiCG3zOmyYx9cjgM1mOYkxFCVZJBmV-2IF_fofdhjj5fZwRAdiUqUWXq-wvlYkgpYvdqhjPznJP5l1OGv7y1_4r-TQWeAHkrjOk</recordid><startdate>20190729</startdate><enddate>20190729</enddate><creator>Janipour, Mohsen</creator><creator>Misirlioglu, I Burc</creator><creator>Sendur, Kursat</creator><general>MDPI AG</general><general>MDPI</general><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SR</scope><scope>8FD</scope><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>D1I</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>JG9</scope><scope>KB.</scope><scope>PDBOC</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>7X8</scope><scope>5PM</scope><orcidid>https://orcid.org/0000-0003-3210-7542</orcidid></search><sort><creationdate>20190729</creationdate><title>A Theoretical Treatment of THz Resonances in Semiconductor GaAs p-n Junctions</title><author>Janipour, Mohsen ; Misirlioglu, I Burc ; Sendur, Kursat</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c406t-c89e530961f607cb14bc4e00f8c7453a8123f0aacd3f55ee6ac93607a6fdd8b3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2019</creationdate><topic>Carrier density</topic><topic>Current carriers</topic><topic>Damping</topic><topic>Doping</topic><topic>Electric fields</topic><topic>Electron mass</topic><topic>Gallium arsenide</topic><topic>Heterostructures</topic><topic>Infrared radiation</topic><topic>Integrated circuits</topic><topic>Light emitting diodes</topic><topic>Majority carriers</topic><topic>Materials selection</topic><topic>Metals</topic><topic>Metamaterials</topic><topic>Modulators</topic><topic>Multilayers</topic><topic>Organic light emitting diodes</topic><topic>P-n junctions</topic><topic>Photovoltaic cells</topic><topic>Propagation</topic><topic>Quantum dots</topic><topic>Relaxation time</topic><topic>Semiconductor lasers</topic><topic>Semiconductors</topic><topic>Solar cells</topic><topic>Terahertz frequencies</topic><topic>Waveguides</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Janipour, Mohsen</creatorcontrib><creatorcontrib>Misirlioglu, I Burc</creatorcontrib><creatorcontrib>Sendur, Kursat</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>Engineered Materials Abstracts</collection><collection>Technology Research Database</collection><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>Materials Science & Engineering Collection</collection><collection>ProQuest Central (Alumni Edition)</collection><collection>ProQuest Central UK/Ireland</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Materials Science Collection</collection><collection>ProQuest Central Korea</collection><collection>SciTech Premium Collection</collection><collection>Materials Research Database</collection><collection>Materials Science Database</collection><collection>Materials Science Collection</collection><collection>Publicly Available Content Database</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central China</collection><collection>MEDLINE - Academic</collection><collection>PubMed Central (Full Participant titles)</collection><jtitle>Materials</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Janipour, Mohsen</au><au>Misirlioglu, I Burc</au><au>Sendur, Kursat</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>A Theoretical Treatment of THz Resonances in Semiconductor GaAs p-n Junctions</atitle><jtitle>Materials</jtitle><addtitle>Materials (Basel)</addtitle><date>2019-07-29</date><risdate>2019</risdate><volume>12</volume><issue>15</issue><spage>2412</spage><pages>2412-</pages><issn>1996-1944</issn><eissn>1996-1944</eissn><abstract>Semiconductor heterostructures are suitable for the design and fabrication of terahertz (THz) plasmonic devices, due to their matching carrier densities. The classical dispersion relations in the current literature are derived for metal plasmonic materials, such as gold and silver, for which a homogeneous dielectric function is valid. Penetration of the electric fields into semiconductors induces locally varying charge densities and a spatially varying dielectric function is expected. While such an occurrence renders tunable THz plasmonics a possibility, it is crucial to understand the conditions under which propagating resonant conditions for the carriers occur, upon incidence of an electromagnetic radiation. In this manuscript, we derive a dispersion relation for a p-n heterojunction and apply the methodology to a GaAs p-n junction, a material of interest for optoelectronic devices. Considering symmetrically doped p- and n-type regions with equal width, the effect of certain parameters (such as doping and voltage bias) on the dispersion curve of the p-n heterojunction were investigated. Keeping in sight the different effective masses and mobilities of the carriers, we were able to obtain the conditions that yield identical dielectric functions for the p- and n-regions. Our results indicated that the p-n GaAs system can sustain propagating resonances and can be used as a layered plasmonic waveguide. The conditions under which this is feasible fall in the frequency region between the transverse optical phonon resonance of GaAs and the traditional cut-off frequency of the diode waveguide. In addition, our results indicated when the excitation was slightly above the phonon resonance frequency, the plasmon propagation attained low-loss characteristics. We also showed that the existence or nonexistence of the depletion zone between the p- and n- interfaces allowed certain plasmon modes to propagate, while others decayed rapidly, pointing out the possibility for a design of selective filters.</abstract><cop>Switzerland</cop><pub>MDPI AG</pub><pmid>31362342</pmid><doi>10.3390/ma12152412</doi><orcidid>https://orcid.org/0000-0003-3210-7542</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | Carrier density Current carriers Damping Doping Electric fields Electron mass Gallium arsenide Heterostructures Infrared radiation Integrated circuits Light emitting diodes Majority carriers Materials selection Metals Metamaterials Modulators Multilayers Organic light emitting diodes P-n junctions Photovoltaic cells Propagation Quantum dots Relaxation time Semiconductor lasers Semiconductors Solar cells Terahertz frequencies Waveguides |
title | A Theoretical Treatment of THz Resonances in Semiconductor GaAs p-n Junctions |
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