2017
DOI: 10.1016/j.jmaa.2017.05.053
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Uniform resolvent estimates and absence of eigenvalues for Lamé operators with complex potentials

Abstract: We consider the 0-order perturbed Lamé operator −∆ * +V (x). It is well known that if one considers the free case, namely V = 0, the spectrum of −∆ * is purely continuous and coincides with the non-negative semi-axis. The first purpose of the paper is to show that, at least in part, this spectral property is preserved in the perturbed setting. Precisely, developing a suitable multipliers technique, we will prove the absence of point spectrum for Lamé operator with potentials which satisfy a variational inequal… Show more

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Cited by 19 publications
(25 citation statements)
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“…The two-dimensional situation was covered later in [15]. The robustness of the method of multipliers has been demonstrated in its successful application to the half-space instead of the whole Euclidean space in [4] and to Lamé instead of Schrödinger operators in [3]. In the present paper, we push the analysis forward by investigating how the unconventional method provides meaningful and interesting results in the same direction also in the less explored setting of the spinorial Hamiltonians.…”
Section: Objectives and State Of The Artmentioning
confidence: 87%
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“…The two-dimensional situation was covered later in [15]. The robustness of the method of multipliers has been demonstrated in its successful application to the half-space instead of the whole Euclidean space in [4] and to Lamé instead of Schrödinger operators in [3]. In the present paper, we push the analysis forward by investigating how the unconventional method provides meaningful and interesting results in the same direction also in the less explored setting of the spinorial Hamiltonians.…”
Section: Objectives and State Of The Artmentioning
confidence: 87%
“…Let A ∈ L 2 loc (R 3 ; R 3 ) be such that B ∈ L 2 loc (R 3 ; R 3 ). Suppose that V ∈ L 1 loc (R 3 ; C 2×2 ) admits the decomposition V = V (1) (2) with components V (1) ∈ L 1 loc (R 3 ) and V (2) = V (2) I C 2 , where V (2) ∈ L 1 loc (R 3 ) is such that [∂ r (r Re V (2) )] + ∈ L 1 loc (R 3 ) and r V (1) , r (Re V (2) ) − , r Im V (2) ∈ L 2 loc (R 3 ). such that, for all two-vector u with components in C ∞ 0 (R 3 ), the inequalities…”
Section: Theorem 11 (Spinor Schrödinger Equation)mentioning
confidence: 99%
“…Concerning the Schrödinger equation we should quote [14,16,20,21] and for the Dirac equation [9,10]. Moreover, we mention [15] for an adaptation of this method to an elasticity setting.…”
Section: Preliminariesmentioning
confidence: 99%
“…Moreover, in [20] the two-dimensional electromagnetic Schrödinger operators has been covered by the same authors. We also mention [15] where an adaptation of this method to an elasticity setting was performed by the first author.…”
Section: Introductionmentioning
confidence: 99%
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