On the One-Dimensional Current Driven Semiconductor Equations

The steady state semiconductor equations in one dimension are examined subject to a given current through the device, supplemented by Dirichlet boundary conditions on one end of the device. Solutions to this current driven model are identified as the fixed points of a mapping T, and uniqueness of so...

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Published inSIAM journal on applied mathematics Vol. 51; no. 3; pp. 748 - 774
Main Author Kerkhoven, Thomas
Format Journal Article
LanguageEnglish
Published Philadelphia, PA Society for Industrial and Applied Mathematics 01.06.1991
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Abstract The steady state semiconductor equations in one dimension are examined subject to a given current through the device, supplemented by Dirichlet boundary conditions on one end of the device. Solutions to this current driven model are identified as the fixed points of a mapping T, and uniqueness of solutions for the unipolar model is shown for arbitrary currents, by demonstrating that T is unconditionally a contraction. For both the uni- and the bipolar model existence of solutions close to thermodynamic equilibrium is shown. This means that for the one-dimensional unipolar current driven model the situation is complementary to that for the potential driven model where it is possible to show existence of solutions for arbitrary applied potentials, and uniqueness close to thermodynamic equilibrium only. For the unipolar case, iteration with the mapping T defines an algorithm for the solution of this model which is unconditionally convergent to the unique solution if it exists.
AbstractList The steady state semiconductor equations in one dimension are examined subject to a given current through the device, supplemented by Dirichlet boundary conditions on one end of the device. Solutions to this current driven model are identified as the fixed points of a mapping $T$, and uniqueness of solutions for the unipolar model is shown for arbitrary currents, by demonstrating that $T$ is unconditionally a contraction. For both the uni-and the bipolar model existence of solutions close to thermodynamic equilibrium is shown. This means that for the one-dimensional unipolar current driven model the situation is complementary to that for the potential driven model where it is possible to show existence of solutions for arbitrary applied potentials, and uniqueness close to thermodynamic equilibrium only. For the unipolar case, iteration with the mapping $T$ defines an algorithm for the solution of this model which is unconditionally convergent to the unique solution if it exists.
Author Kerkhoven, Thomas
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CitedBy_id crossref_primary_10_1090_S0002_9947_96_01519_X
crossref_primary_10_1137_S003614109018823X
crossref_primary_10_1016_j_matcom_2004_01_012
crossref_primary_10_1080_00036819908840733
crossref_primary_10_1016_0362_546X_92_90227_6
crossref_primary_10_1016_j_jmaa_2006_10_022
Cites_doi 10.1137/0145034
10.1007/978-3-642-61798-0
10.1016/0038-1101(72)90043-3
10.1103/PhysRev.87.835
10.1103/PhysRev.87.387
10.1137/0909005
10.1016/0362-546X(80)90097-8
10.1007/978-3-7091-3678-2
10.1137/0723076
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Copyright Copyright 1991 Society for Industrial and Applied Mathematics
1992 INIST-CNRS
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Issue 3
Keywords Transport process
Unipolar
Semiconductor materials
Differential equation
Charge carrier recombination
One dimensional model
Theoretical study
Charge carrier generation
Equation
Equation resolution
Boundary condition
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SubjectTerms A priori knowledge
Boundary conditions
Condensed matter: electronic structure, electrical, magnetic, and optical properties
Conduction electrons
Contact potentials
Continuity equations
Doping
Electric current
Electronic transport in condensed matter
Electrons
Equilibrium
Exact sciences and technology
Ordinary differential equations
Physics
Semiconductors
Simulation
Theory of electronic transport; scattering mechanisms
Uniqueness
Title On the One-Dimensional Current Driven Semiconductor Equations
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Volume 51
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