Simulating and modeling the breakdown voltage in a semi-insulating GaAs P+N junction diode
This work aims to determine the characteristic PN junction diode, subject to a reverse polarization, while I (breakdown voltage) of the inverse current in a GaAs specifying the parameters that influence the breakdown voltage of the diode. In this work, we simulated the behavior of the ionization phe...
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Published in | Journal of semiconductors Vol. 35; no. 8; pp. 60 - 68 |
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Main Authors | , , |
Format | Journal Article |
Language | English |
Published |
01.08.2014
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Subjects | |
Online Access | Get full text |
ISSN | 1674-4926 |
DOI | 10.1088/1674-4926/35/8/084002 |
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Abstract | This work aims to determine the characteristic PN junction diode, subject to a reverse polarization, while I (breakdown voltage) of the inverse current in a GaAs specifying the parameters that influence the breakdown voltage of the diode. In this work, we simulated the behavior of the ionization phenomenon by impact breakdown by avalanche of the PN junctions, subject to an inverse polarization. We will take into account both the trapping model in a stationary regime in the P+N structure using like material of basis the Ⅲ-Ⅴ compounds and mainly the GaAs semi-insulating in which the deep centers have in important densities. We are talking about the model of trapping in the space charge region (SCR) and that is the trap density donor and acceptor states. The carrier crossing the space charge region (SCR) of W thickness creates N electron-hole pairs: for every created pair, the electron and the hole are swept quickly by the electric field, each in an opposite direction, which comes back, according to an already accepted reasoning, to the crossing of the space charge region (SCR) by an electron or a hole. So the even N pair created by the initial particle provoke N2 ionizations and so forth. The study of the physical and electrical behaviour of semiconductors is based on the influence of the presence of deep centers on the characteristic I(V) current-tension, which requires the calculation of the electrostatic potential, the electric field, the integral of ionization, the density of the states traps, the diffusion current of minority in the regions (1) and (3), the current thermal generation in the region (2), the leakage current in the surface, and the breakdown voltage. |
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AbstractList | This work aims to determine the characteristic PN junction diode, subject to a reverse polarization, while I (breakdown voltage) of the inverse current in a GaAs specifying the parameters that influence the breakdown voltage of the diode. In this work, we simulated the behavior of the ionization phenomenon by impact breakdown by avalanche of the PN junctions, subject to an inverse polarization. We will take into account both the trapping model in a stationary regime in the P+N structure using like material of basis the Ⅲ-Ⅴ compounds and mainly the GaAs semi-insulating in which the deep centers have in important densities. We are talking about the model of trapping in the space charge region (SCR) and that is the trap density donor and acceptor states. The carrier crossing the space charge region (SCR) of W thickness creates N electron-hole pairs: for every created pair, the electron and the hole are swept quickly by the electric field, each in an opposite direction, which comes back, according to an already accepted reasoning, to the crossing of the space charge region (SCR) by an electron or a hole. So the even N pair created by the initial particle provoke N2 ionizations and so forth. The study of the physical and electrical behaviour of semiconductors is based on the influence of the presence of deep centers on the characteristic I(V) current-tension, which requires the calculation of the electrostatic potential, the electric field, the integral of ionization, the density of the states traps, the diffusion current of minority in the regions (1) and (3), the current thermal generation in the region (2), the leakage current in the surface, and the breakdown voltage. |
Author | A. Resfa Brahimi. R. Menezla M. Benchhima |
AuthorAffiliation | Laboratory of Modeling and Conception of the Circuits Electronic, Department of Electronics, University Djillali Liab6s, BP89.Sidi Bel Abbes 22000, Algeria |
Author_xml | – sequence: 1 givenname: A. surname: Resfa fullname: Resfa, A. – sequence: 2 givenname: Brahimi R. surname: Menezla fullname: Menezla, Brahimi R. – sequence: 3 givenname: M. surname: Benchhima fullname: Benchhima, M. |
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Cites_doi | 10.1103/PhysRev.109.1537 10.1063/1.106950 10.1103/PhysRev.99.1234 10.1016/0038-1101(74)90011-2 10.1063/1.1754511 10.1016/0038-1101(82)90077-6 10.1016/0038-1101(70)90139-5 10.1063/1.91431 10.1016/0038-1101(67)90111-6 10.1016/0038-1101(76)90152-0 10.1063/1.334178 10.1109/T-ED.1978.19263 10.1016/0038-1101(72)90070-6 10.1051/rphysap:019780013012067300 10.1103/PhysRev.134.A761 |
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Notes | This work aims to determine the characteristic PN junction diode, subject to a reverse polarization, while I (breakdown voltage) of the inverse current in a GaAs specifying the parameters that influence the breakdown voltage of the diode. In this work, we simulated the behavior of the ionization phenomenon by impact breakdown by avalanche of the PN junctions, subject to an inverse polarization. We will take into account both the trapping model in a stationary regime in the P+N structure using like material of basis the Ⅲ-Ⅴ compounds and mainly the GaAs semi-insulating in which the deep centers have in important densities. We are talking about the model of trapping in the space charge region (SCR) and that is the trap density donor and acceptor states. The carrier crossing the space charge region (SCR) of W thickness creates N electron-hole pairs: for every created pair, the electron and the hole are swept quickly by the electric field, each in an opposite direction, which comes back, according to an already accepted reasoning, to the crossing of the space charge region (SCR) by an electron or a hole. So the even N pair created by the initial particle provoke N2 ionizations and so forth. The study of the physical and electrical behaviour of semiconductors is based on the influence of the presence of deep centers on the characteristic I(V) current-tension, which requires the calculation of the electrostatic potential, the electric field, the integral of ionization, the density of the states traps, the diffusion current of minority in the regions (1) and (3), the current thermal generation in the region (2), the leakage current in the surface, and the breakdown voltage. 11-5781/TN the phenomenon of ionization by impact; the integrals of ionizations In and Ip; the potential elec-trostatic and electric field; variation of the trap state density Art; the integral of ionization reversecurrent-breakdown voltage; the current-breakdown voltage characteristics of the P+N junction diode |
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PublicationTitle | Journal of semiconductors |
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References | Fulop W (13) 1967; 10 23 Brahimi R M (3) 1995 25 26 Miller S L (20) 1955; 99 Shockley-Read W (11) 1961; B11 Chynoweth A G (18) 1950; 109 Urgell J J (22) 1978; 13 Grove A S (12) 1971 Sze S M (4) 1981 Boisson V (10) 1985 Kittel C (2) 2004; 7917 Vapaille et R Castagné A (9) 1987 14 15 16 17 Amrani M (27) 1996 Leturcq P (24) 1976 Taylor D M (21) 1984; 56 Lee C A (19) 1964; 134 6 7 8 Bonnaud O (5) 1978 Mathieu H (1) 1996 |
References_xml | – year: 1987 ident: 9 publication-title: Semiconductor devices and integrated circuits – year: 1981 ident: 4 publication-title: Book of physics of semiconductor devices – year: 1995 ident: 3 – volume: B11 start-page: 81 issn: 0368-3400 year: 1961 ident: 11 publication-title: J Phys – volume: 109 start-page: 1537 year: 1950 ident: 18 publication-title: Phys Rev doi: 10.1103/PhysRev.109.1537 – ident: 6 doi: 10.1063/1.106950 – volume: 99 start-page: 1234 year: 1955 ident: 20 publication-title: Phys Rev doi: 10.1103/PhysRev.99.1234 – ident: 23 doi: 10.1016/0038-1101(74)90011-2 – year: 1978 ident: 5 – year: 1985 ident: 10 – year: 1996 ident: 27 – ident: 14 doi: 10.1063/1.1754511 – ident: 26 doi: 10.1016/0038-1101(82)90077-6 – volume: 7917 year: 2004 ident: 2 publication-title: Physics of the solid state – ident: 25 doi: 10.1016/0038-1101(70)90139-5 – year: 1996 ident: 1 publication-title: Physics of semiconductors and electronic components – year: 1971 ident: 12 publication-title: Physics and technology of semiconductor devices – ident: 7 doi: 10.1063/1.91431 – volume: 10 start-page: 39 issn: 0038-1101 year: 1967 ident: 13 publication-title: Solid-State Electron doi: 10.1016/0038-1101(67)90111-6 – ident: 16 doi: 10.1016/0038-1101(76)90152-0 – volume: 56 start-page: 1881 year: 1984 ident: 21 publication-title: Appl Phys doi: 10.1063/1.334178 – ident: 8 doi: 10.1016/0038-1101(70)90139-5 – ident: 15 doi: 10.1109/T-ED.1978.19263 – ident: 17 doi: 10.1016/0038-1101(72)90070-6 – year: 1976 ident: 24 – volume: 13 start-page: 673 issn: 0035-1687 year: 1978 ident: 22 publication-title: Rev Phys Appl (Paris) doi: 10.1051/rphysap:019780013012067300 – volume: 134 start-page: 761 year: 1964 ident: 19 publication-title: Phys Rev doi: 10.1103/PhysRev.134.A761 |
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Snippet | This work aims to determine the characteristic PN junction diode, subject to a reverse polarization, while I (breakdown voltage) of the inverse current in a... |
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SubjectTerms | PN结二极管 击穿电压 半绝缘GaAs 扩散电流 模型 模拟 空间电荷区 结型 |
Title | Simulating and modeling the breakdown voltage in a semi-insulating GaAs P+N junction diode |
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