2019
DOI: 10.1002/mana.201800206
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‐Theory for Schrödinger systems

Abstract: In this article, we study for p∈(1,∞) the Lp‐realization of the vector‐valued Schrödinger operator Lu:=prefix div (Q∇u)+Vu. Using a noncommutative version of the Dore–Venni theorem due to Monniaux and Prüss, we prove that the Lp‐realization of scriptL, defined on the intersection of the natural domains of the differential and multiplication operators which form scriptL, generates a strongly continuous contraction semigroup on Lp(double-struckRd;double-struckCm). We also study additional properties of the semig… Show more

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Cited by 13 publications
(34 citation statements)
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“…An easy scalar one-dimensional counterexample shows that, even in the case when the diffusion coefficient of the operator A is constant and the drift grows slightly more than linearly at infinity, there exists no realization of the operator A in L p (ℝ) which generates a strongly continuous or an analytic semigroup (see [34]). Similar pathological behaviors are exhibited in the vector-valued case (see, e.g., [22,Example 2.2], [25,Example 2.3], [9,Sect. 3]).…”
Section: Remark 32supporting
confidence: 59%
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“…An easy scalar one-dimensional counterexample shows that, even in the case when the diffusion coefficient of the operator A is constant and the drift grows slightly more than linearly at infinity, there exists no realization of the operator A in L p (ℝ) which generates a strongly continuous or an analytic semigroup (see [34]). Similar pathological behaviors are exhibited in the vector-valued case (see, e.g., [22,Example 2.2], [25,Example 2.3], [9,Sect. 3]).…”
Section: Remark 32supporting
confidence: 59%
“…To the best of our knowledge, this is the first paper aimed at providing a precise characterization of the domain of the infinitesimal generator of the associated semigroup, when also the diffusion coefficients of the operator A are possibly unbounded and the operator is coupled up to the first order. Indeed, the description of the domain of the generator of operator A in L p (ℝ d ;ℝ m ) has been provided only in the papers [22,25,28], but there the coefficients of the diffusion part are bounded, and in [7,8] where there is no coupling in the first-order term.…”
Section: Introductionmentioning
confidence: 99%
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