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1.
Multiparameter maximal estimates are considered for operators of Schrödinger type. Sharp and almost sharp results, that extend work by Rogers and Villarroya, are obtained. We provide new estimates via the integrability of the kernel which naturally appears with a TT? argument and discuss the behavior at the endpoints. We treat in particular the case of global integrability of the maximal operator on finite time for solutions to the linear Schrödinger equation and make some comments on an open problem. 相似文献
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We consider Schrödinger operators with periodic potentials on periodic discrete graphs. The spectrum of the Schrödinger operator consists of an absolutely continuous part (a union of a finite number of non-degenerated bands) plus a finite number of flat bands, i.e., eigenvalues of infinite multiplicity. We obtain estimates of the Lebesgue measure of the spectrum in terms of geometric parameters of the graph and show that they become identities for some class of graphs. Moreover, we obtain stability estimates and show the existence and positions of large number of flat bands for specific graphs. The proof is based on the Floquet theory and the precise representation of fiber Schrödinger operators, constructed in the paper. 相似文献
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Mouez Dimassi 《Journal of Functional Analysis》2005,225(1):193-228
We study the spectral shift function s(λ,h) and the resonances of the operator P(h)=-Δ+V(x)+W(hx). Here V is a periodic potential, W a decreasing perturbation and h a small positive constant. We give a representation of the derivative of s(λ,h) related to the resonances of P(h), and we obtain a Weyl-type asymptotics of s(λ,h). We establish an upper bound O(h-n+1) for the number of the resonances of P(h) lying in a disk of radius h. 相似文献
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Luca Fanelli 《Journal of Mathematical Analysis and Applications》2009,357(1):1-420
We prove some uniform in ? a priori estimates for solutions of the equation
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Sergey A. Denisov 《Journal of Functional Analysis》2008,254(8):2186-2226
For a large class of Schrödinger operators, we introduce the hyperbolic quadratic pencils by making the coupling constant dependent on the energy in the very special way. For these pencils, many problems of scattering theory are significantly easier to study. Then, we give some applications to the original Schrödinger operators including one-dimensional Schrödinger operators with L2-operator-valued potentials, multidimensional Schrödinger operators with slowly decaying potentials. 相似文献
7.
In this work we obtain boundedness on weighted Lebesgue spaces on Rd of the semi-group maximal function, Riesz transforms, fractional integrals and g-function associated to the Schrödinger operator −Δ+V, where V satisfies a reverse Hölder inequality with exponent greater than d/2. We consider new classes of weights that locally behave as Muckenhoupt's weights and actually include them. The notion of locality is defined by means of the critical radius function of the potential V given in Shen (1995) [8]. 相似文献
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Ognjen Milatovic 《Journal of Mathematical Analysis and Applications》2009,354(1):125-133
We consider a Schrödinger differential expression P=ΔM+V on a complete Riemannian manifold (M,g) with metric g, where ΔM is the scalar Laplacian on M and V is a real-valued locally integrable function on M. We study two self-adjoint realizations of P in L2(M) and show their equality. This is an extension of a result of S. Agmon. 相似文献
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We prove that one-dimensional reflectionless Schrödinger operators with spectrum a homogeneous set in the sense of Carleson, belonging to the class introduced by Sodin and Yuditskii, have purely absolutely continuous spectra. This class includes all earlier examples of reflectionless almost periodic Schrödinger operators. In addition, we construct examples of reflectionless Schrödinger operators with more general types of spectra, given by the complement of a Denjoy-Widom-type domain in C, which exhibit a singular component. 相似文献
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Attila B. von Keviczky Richard L. Hall 《Journal of Mathematical Analysis and Applications》2004,292(1):274-293
The Friedrichs extension for the generalized spiked harmonic oscillator given by the singular differential operator −d2/dx2+Bx2+Ax−2+λx−α (B>0, A?0) in L2(0,∞) is studied. We look at two different domains of definition for each of these differential operators in L2(0,∞), namely C0∞(0,∞) and D(T2,F)∩D(Mλ,α), where the latter is a subspace of the Sobolev space W2,2(0,∞). Adjoints of these differential operators on C0∞(0,∞) exist as result of the null-space properties of functionals. For the other domain, convolutions and Jensen and Minkowski integral inequalities, density of C0∞(0,∞) in D(T2,F)∩D(Mλ,α) in L2(0,∞) lead to the other adjoints. Further density properties C0∞(0,∞) in D(T2,F)∩D(Mλ,α) yield the Friedrichs extension of these differential operators with domains of definition D(T2,F)∩D(Mλ,α). 相似文献
13.
Pavel Kurasov 《Journal of Functional Analysis》2008,254(4):934-953
The inverse spectral problem for Schrödinger operators on finite compact metric graphs is investigated. The relations between the spectral asymptotics and geometric properties of the underlying graph are studied. It is proven that the Euler characteristic of the graph can be calculated from the spectrum of the Schrödinger operator in the case of essentially bounded real potentials and standard boundary conditions at the vertices. Several generalizations of the presented results are discussed. 相似文献
14.
Kwang C. Shin 《Journal of Mathematical Analysis and Applications》2004,299(1):19-39
Recently, a trace formula for non-self-adjoint periodic Schrödinger operators in L2(R) associated with Dirichlet eigenvalues was proved in [Differential Integral Equations 14 (2001) 671-700]. Here we prove a corresponding trace formula associated with Neumann eigenvalues. In addition we investigate Dirichlet and Neumann eigenvalues of such operators. In particular, using the Dirichlet and Neumann trace formulas, we provide detailed information on location of the Dirichlet and Neumann eigenvalues for the model operator with the potential Ke2ix, where K∈C. 相似文献
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Brice Camus 《Journal of Differential Equations》2006,226(1):295-322
We study the semi-classical trace formula at a critical energy level for a Schrödinger operator on Rn. We assume here that the potential has a totally degenerate critical point associated to a local maximum. The main result, which establishes the contribution of the associated equilibrium in the trace formula, is valid for all time in a compact subset of R and includes the singularity in t=0. For these new contributions the asymptotic expansion involves the logarithm of the parameter h. Depending on an explicit arithmetic condition on the dimension and the order of the critical point, this logarithmic contribution can appear in the leading term. 相似文献
16.
B. Helffer 《Journal of Functional Analysis》2009,257(10):3043-3081
We consider a periodic magnetic Schrödinger operator Hh, depending on the semiclassical parameter h>0, on a noncompact Riemannian manifold M such that H1(M,R)=0 endowed with a properly discontinuous cocompact isometric action of a discrete group. We assume that there is no electric field and that the magnetic field has a periodic set of compact magnetic wells. We suppose that the magnetic field vanishes regularly on a hypersurface S. First, we prove upper and lower estimates for the bottom λ0(Hh) of the spectrum of the operator Hh in L2(M). Then, assuming the existence of non-degenerate miniwells for the reduced spectral problem on S, we prove the existence of an arbitrarily large number of spectral gaps for the operator Hh in the region close to λ0(Hh), as h→0. In this case, we also obtain upper estimates for the eigenvalues of the one-well problem. 相似文献
17.
It is shown that the notion of trace induced by a given complete orthonormal system relates the Skorohod integral with a corresponding Ogawa‐type integral evaluated with respect to the same orthonormal systems. Similarly the multiple Wiener‐Ito integral is shown to be related to a multiple Ogawa‐type integral induced by a complete orthonormal system via the Hu‐Meyer formula with suitably defined multiple traces. The notion of skeleton of a Wiener functional relative to a given orthonormal system is defined and yields what seems to be a “natural” extension of Wiener functionals to the Cameron Martin space and the Wiener processes with a different scale. 相似文献
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Gülen Ba?canbaz-Tunca 《Journal of Mathematical Analysis and Applications》2003,286(1):207-219
In this paper we investigate the spectrum and the spectral singularities of an operator L generalized in by the differential expression
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In this paper we study the existence of a first zero and the oscillatory behavior of solutions of the ordinary differential equation ′(vz′)+Avz=0, where A, v are functions arising from geometry. In particular, we introduce a new technique to estimate the distance between two consecutive zeros. These results are applied in the setting of complete Riemannian manifolds: in particular, we prove index bounds for certain Schrödinger operators, and an estimate of the growth of the spectral radius of the Laplacian outside compact sets when the volume growth is faster than exponential. Applications to the geometry of complete minimal hypersurfaces of Euclidean space, to minimal surfaces and to the Yamabe problem are discussed. 相似文献
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Ahmad El Soufi Nazih Moukadem 《Journal of Mathematical Analysis and Applications》2006,314(1):195-209
Let M be a compact Riemannian manifold with or without boundary, and let −Δ be its Laplace-Beltrami operator. For any bounded scalar potential q, we denote by λi(q) the ith eigenvalue of the Schrödinger type operator −Δ+q acting on functions with Dirichlet or Neumann boundary conditions in case ∂M≠∅. We investigate critical potentials of the eigenvalues λi and the eigenvalue gaps Gij=λj−λi considered as functionals on the set of bounded potentials having a given mean value on M. We give necessary and sufficient conditions for a potential q to be critical or to be a local minimizer or a local maximizer of these functionals. For instance, we prove that a potential q∈L∞(M) is critical for the functional λ2 if and only if q is smooth, λ2(q)=λ3(q) and there exist second eigenfunctions f1,…,fk of −Δ+q such that . In particular, λ2 (as well as any λi) admits no critical potentials under Dirichlet boundary conditions. Moreover, the functional λ2 never admits locally minimizing potentials. 相似文献