A complete multifluid model for bipolar semiconductors, with interacting carriers, phonons, and photons
If electrons (e) and holes (h) in metals or semiconductors are heated to the temperatures T e and T h greater than the lattice temperature, the electron–phonon interaction causes energy relaxation. In the non-uniform case a momentum relaxation occurs as well. In view of such an application, a new mo...
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description | If electrons (e) and holes (h) in metals or semiconductors are heated to the temperatures
T
e
and
T
h
greater than the lattice temperature, the electron–phonon interaction causes energy relaxation. In the non-uniform case a momentum relaxation occurs as well. In view of such an application, a new model, based on an asymptotic procedure for solving the kinetic equations of carriers, phonons, and photons, is proposed, which gives naturally the displaced Maxwellian at the leading order. Several generation–recombination (GR) events occur in bipolar semiconductors. In the presence of photons the most important ones are the radiative GR events, direct, indirect, and exciton-catalyzed. Phonons and photons are treated here as a participating species, with their own equation. All the phonon–photon interactions are accounted for. Moreover, carrier–photon (Compton) interactions are introduced, which make complete the model. After that, balance equations for the electron number, hole number, energy densities, and momentum densities are constructed, which constitute now a system of macroscopic equations for the chemical potentials (carriers), the temperatures (carriers and bosons), and the drift velocities (carriers and bosons). In the drift–diffusion approximation the constitutive laws are derived and the Onsager relations recovered, even in the presence of an external magnetic field. |
doi_str_mv | 10.1007/s00033-017-0875-8 |
format | Article |
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T
e
and
T
h
greater than the lattice temperature, the electron–phonon interaction causes energy relaxation. In the non-uniform case a momentum relaxation occurs as well. In view of such an application, a new model, based on an asymptotic procedure for solving the kinetic equations of carriers, phonons, and photons, is proposed, which gives naturally the displaced Maxwellian at the leading order. Several generation–recombination (GR) events occur in bipolar semiconductors. In the presence of photons the most important ones are the radiative GR events, direct, indirect, and exciton-catalyzed. Phonons and photons are treated here as a participating species, with their own equation. All the phonon–photon interactions are accounted for. Moreover, carrier–photon (Compton) interactions are introduced, which make complete the model. After that, balance equations for the electron number, hole number, energy densities, and momentum densities are constructed, which constitute now a system of macroscopic equations for the chemical potentials (carriers), the temperatures (carriers and bosons), and the drift velocities (carriers and bosons). In the drift–diffusion approximation the constitutive laws are derived and the Onsager relations recovered, even in the presence of an external magnetic field.</description><identifier>ISSN: 0044-2275</identifier><identifier>EISSN: 1420-9039</identifier><identifier>DOI: 10.1007/s00033-017-0875-8</identifier><language>eng</language><publisher>Cham: Springer International Publishing</publisher><subject>Asymptotic methods ; Bosons ; Displacements (lattice) ; Drift ; Engineering ; Kinetic equations ; Macroscopic equations ; Mathematical Methods in Physics ; Mathematical models ; Phonons ; Photons ; Semiconductors ; Theoretical and Applied Mechanics</subject><ispartof>Zeitschrift für angewandte Mathematik und Physik, 2017-12, Vol.68 (6), p.1-18, Article 130</ispartof><rights>Springer International Publishing AG 2017</rights><rights>Copyright Springer Science & Business Media 2017</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c268t-90d4bafecae4a2cdb7842132dfaacc171335073a9ec582967166887f3fe8d2063</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.1007/s00033-017-0875-8$$EPDF$$P50$$Gspringer$$H</linktopdf><linktohtml>$$Uhttps://link.springer.com/10.1007/s00033-017-0875-8$$EHTML$$P50$$Gspringer$$H</linktohtml><link.rule.ids>314,780,784,27924,27925,41488,42557,51319</link.rule.ids></links><search><creatorcontrib>Rossani, A.</creatorcontrib><title>A complete multifluid model for bipolar semiconductors, with interacting carriers, phonons, and photons</title><title>Zeitschrift für angewandte Mathematik und Physik</title><addtitle>Z. Angew. Math. Phys</addtitle><description>If electrons (e) and holes (h) in metals or semiconductors are heated to the temperatures
T
e
and
T
h
greater than the lattice temperature, the electron–phonon interaction causes energy relaxation. In the non-uniform case a momentum relaxation occurs as well. In view of such an application, a new model, based on an asymptotic procedure for solving the kinetic equations of carriers, phonons, and photons, is proposed, which gives naturally the displaced Maxwellian at the leading order. Several generation–recombination (GR) events occur in bipolar semiconductors. In the presence of photons the most important ones are the radiative GR events, direct, indirect, and exciton-catalyzed. Phonons and photons are treated here as a participating species, with their own equation. All the phonon–photon interactions are accounted for. Moreover, carrier–photon (Compton) interactions are introduced, which make complete the model. After that, balance equations for the electron number, hole number, energy densities, and momentum densities are constructed, which constitute now a system of macroscopic equations for the chemical potentials (carriers), the temperatures (carriers and bosons), and the drift velocities (carriers and bosons). In the drift–diffusion approximation the constitutive laws are derived and the Onsager relations recovered, even in the presence of an external magnetic field.</description><subject>Asymptotic methods</subject><subject>Bosons</subject><subject>Displacements (lattice)</subject><subject>Drift</subject><subject>Engineering</subject><subject>Kinetic equations</subject><subject>Macroscopic equations</subject><subject>Mathematical Methods in Physics</subject><subject>Mathematical models</subject><subject>Phonons</subject><subject>Photons</subject><subject>Semiconductors</subject><subject>Theoretical and Applied Mechanics</subject><issn>0044-2275</issn><issn>1420-9039</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2017</creationdate><recordtype>article</recordtype><recordid>eNp1kEtLxDAUhYMoOD5-gLuAW6t5NE26HAZfMOBG1yGTx0yGtqlJivjvTakLN67uvdxzzr18ANxgdI8R4g8JIURphTCvkOCsEidghWuCqhbR9hSsEKrrihDOzsFFSsei5hjRFdivoQ792NlsYT912btu8gb2wdgOuhDhzo-hUxEm23sdBjPpHGK6g18-H6Afso1KZz_soVYxejuvxkMYwlAaNZh5yGW4AmdOdcle_9ZL8PH0-L55qbZvz6-b9bbSpBG5fGvqnXJWK1sros2Oi5pgSoxTSmvMMaUMcapaq5kgbcNx0wjBHXVWGIIaeglul9wxhs_JpiyPYYpDOSlxyxgTjFJeVHhR6RhSitbJMfpexW-JkZx5yoWnLDzlzFOK4iGLJxXtsLfxT_K_ph8fPHmW</recordid><startdate>20171201</startdate><enddate>20171201</enddate><creator>Rossani, A.</creator><general>Springer International Publishing</general><general>Springer Nature B.V</general><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>20171201</creationdate><title>A complete multifluid model for bipolar semiconductors, with interacting carriers, phonons, and photons</title><author>Rossani, A.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c268t-90d4bafecae4a2cdb7842132dfaacc171335073a9ec582967166887f3fe8d2063</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2017</creationdate><topic>Asymptotic methods</topic><topic>Bosons</topic><topic>Displacements (lattice)</topic><topic>Drift</topic><topic>Engineering</topic><topic>Kinetic equations</topic><topic>Macroscopic equations</topic><topic>Mathematical Methods in Physics</topic><topic>Mathematical models</topic><topic>Phonons</topic><topic>Photons</topic><topic>Semiconductors</topic><topic>Theoretical and Applied Mechanics</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Rossani, A.</creatorcontrib><collection>CrossRef</collection><jtitle>Zeitschrift für angewandte Mathematik und Physik</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Rossani, A.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>A complete multifluid model for bipolar semiconductors, with interacting carriers, phonons, and photons</atitle><jtitle>Zeitschrift für angewandte Mathematik und Physik</jtitle><stitle>Z. Angew. Math. Phys</stitle><date>2017-12-01</date><risdate>2017</risdate><volume>68</volume><issue>6</issue><spage>1</spage><epage>18</epage><pages>1-18</pages><artnum>130</artnum><issn>0044-2275</issn><eissn>1420-9039</eissn><abstract>If electrons (e) and holes (h) in metals or semiconductors are heated to the temperatures
T
e
and
T
h
greater than the lattice temperature, the electron–phonon interaction causes energy relaxation. In the non-uniform case a momentum relaxation occurs as well. In view of such an application, a new model, based on an asymptotic procedure for solving the kinetic equations of carriers, phonons, and photons, is proposed, which gives naturally the displaced Maxwellian at the leading order. Several generation–recombination (GR) events occur in bipolar semiconductors. In the presence of photons the most important ones are the radiative GR events, direct, indirect, and exciton-catalyzed. Phonons and photons are treated here as a participating species, with their own equation. All the phonon–photon interactions are accounted for. Moreover, carrier–photon (Compton) interactions are introduced, which make complete the model. After that, balance equations for the electron number, hole number, energy densities, and momentum densities are constructed, which constitute now a system of macroscopic equations for the chemical potentials (carriers), the temperatures (carriers and bosons), and the drift velocities (carriers and bosons). In the drift–diffusion approximation the constitutive laws are derived and the Onsager relations recovered, even in the presence of an external magnetic field.</abstract><cop>Cham</cop><pub>Springer International Publishing</pub><doi>10.1007/s00033-017-0875-8</doi><tpages>18</tpages></addata></record> |
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language | eng |
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source | SpringerNature Journals |
subjects | Asymptotic methods Bosons Displacements (lattice) Drift Engineering Kinetic equations Macroscopic equations Mathematical Methods in Physics Mathematical models Phonons Photons Semiconductors Theoretical and Applied Mechanics |
title | A complete multifluid model for bipolar semiconductors, with interacting carriers, phonons, and photons |
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