2018
DOI: 10.1007/s00033-018-0968-z
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Large time behavior of entropy solutions to one-dimensional unipolar hydrodynamic model for semiconductor devices

Abstract: We are concerned with the global existence and large time behavior of entropy solutions to the one dimensional unipolar hydrodynamic model for semiconductors in the form of Euler-Poisson equations in a bounded interval. In this paper, we first prove the global existence of entropy solution by vanishing viscosity and compensated compactness framework. In particular, the solutions are uniformly bounded with respect to space and time variables by introducing modified Riemann invariants and the theory of invariant… Show more

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Cited by 22 publications
(13 citation statements)
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References 35 publications
(47 reference statements)
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“…which plays a vital role in deriving the upper bound of density, are not trivial in the whole space. This is very different from the bounded domain case considered in [26]. Fortunately, with the help of relative entropy, we obtain our aim.…”
Section: Boundedness Of the Approximate Solutionmentioning
confidence: 90%
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“…which plays a vital role in deriving the upper bound of density, are not trivial in the whole space. This is very different from the bounded domain case considered in [26]. Fortunately, with the help of relative entropy, we obtain our aim.…”
Section: Boundedness Of the Approximate Solutionmentioning
confidence: 90%
“…To extend the local solution to the whole space, it is important to obtain a priori estimate of the upper bound of (n ε , J ε ) and the positive lower estimate of n ε . For γ > 1, as stated in [26], [32], the positive lower bound of n ε can be given by the upper bound estimate of J ε n ε . Therefore, we only need to estimate the bounds of Riemann invariants (w ε , z ε ) to gain the upper bound of (n ε , J ε n ε ).…”
Section: Boundedness Of the Approximate Solutionmentioning
confidence: 99%
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“…for some positive constant C. Remark 6. Theorems 3 and 5 are generalizations of the corresponding theorem of [18], in which the damping coefficient Hðx, tÞ = −1. Suppose α, β, and λ are three positive constants, then Hðx, tÞ = −α/ð1 + tÞ λ − β satisfies all the assumptions of Hðx, tÞ in Theorems 3 and 5.…”
Section: Introductionmentioning
confidence: 99%
“…To the best of our knowledge, for the isothermal flow, the uniform bound for the approximate solutions depends on time t in all the previous results. We remark that the method in our paper can be applied to obtain the existence of weak solutions of related gas dynamic models, such as Euler-Poisson for a semiconductor model [15] or an Euler equation with geometric source terms [13], and may also shed light on the large time behavior of entropy solutions. Besides, we avoid a laborious numerical scheme to construct approximate solutions.…”
Section: Introductionmentioning
confidence: 99%