2,818 research outputs found
Principal Solutions Revisited
The main objective of this paper is to identify principal solutions
associated with Sturm-Liouville operators on arbitrary open intervals , as introduced by Leighton and Morse in the scalar
context in 1936 and by Hartman in the matrix-valued situation in 1957, with
Weyl-Titchmarsh solutions, as long as the underlying Sturm-Liouville
differential expression is nonoscillatory (resp., disconjugate or bounded from
below near an endpoint) and in the limit point case at the endpoint in
question. In addition, we derive an explicit formula for Weyl-Titchmarsh
functions in this case (the latter appears to be new in the matrix-valued
context).Comment: 27 pages, expanded Sect. 2, added reference
Abstract kinetic equations with positive collision operators
We consider "forward-backward" parabolic equations in the abstract form , , where and are
operators in a Hilbert space such that , , and
. The following theorem is proved: if the operator is
similar to a self-adjoint operator, then associated half-range boundary
problems have unique solutions. We apply this theorem to corresponding
nonhomogeneous equations, to the time-independent Fokker-Plank equation , , , as well as to
other parabolic equations of the "forward-backward" type. The abstract kinetic
equation , where is injective and
satisfies a certain positivity assumption, is considered also.Comment: 20 pages, LaTeX2e, version 2, references have been added, changes in
the introductio
Direct and inverse spectral theorems for a class of canonical systems with two singular endpoints
Part I of this paper deals with two-dimensional canonical systems
, , whose Hamiltonian is non-negative and
locally integrable, and where Weyl's limit point case takes place at both
endpoints and . We investigate a class of such systems defined by growth
restrictions on H towards a. For example, Hamiltonians on of the
form where
are included in this class. We develop a direct and inverse spectral theory
parallel to the theory of Weyl and de Branges for systems in the limit circle
case at . Our approach proceeds via - and is bound to - Pontryagin space
theory. It relies on spectral theory and operator models in such spaces, and on
the theory of de Branges Pontryagin spaces.
The main results concerning the direct problem are: (1) showing existence of
regularized boundary values at ; (2) construction of a singular Weyl
coefficient and a scalar spectral measure; (3) construction of a Fourier
transform and computation of its action and the action of its inverse as
integral transforms. The main results for the inverse problem are: (4)
characterization of the class of measures occurring above (positive Borel
measures with power growth at ); (5) a global uniqueness theorem (if
Weyl functions or spectral measures coincide, Hamiltonians essentially
coincide); (6) a local uniqueness theorem.
In Part II of the paper the results of Part I are applied to Sturm--Liouville
equations with singular coefficients. We investigate classes of equations
without potential (in particular, equations in impedance form) and
Schr\"odinger equations, where coefficients are assumed to be singular but
subject to growth restrictions. We obtain corresponding direct and inverse
spectral theorems
Optimal partitioning of an interval and applications to Sturm-Liouville eigenvalues
We study the optimal partitioning of a (possibly unbounded) interval of the
real line into subintervals in order to minimize the maximum of certain
set-functions, under rather general assumptions such as continuity,
monotonicity, and a Radon-Nikodym property. We prove existence and uniqueness
of a solution to this minimax partition problem, showing that the values of the
set-functions on the intervals of any optimal partition must coincide. We also
investigate the asymptotic distribution of the optimal partitions as tends
to infinity. Several examples of set-functions fit in this framework, including
measures, weighted distances and eigenvalues. We recover, in particular, some
classical results of Sturm-Liouville theory: the asymptotic distribution of the
zeros of the eigenfunctions, the asymptotics of the eigenvalues, and the
celebrated Weyl law on the asymptotics of the counting function
What is the optimal shape of a fin for one dimensional heat conduction?
This article is concerned with the shape of small devices used to control the
heat flowing between a solid and a fluid phase, usually called \textsl{fin}.
The temperature along a fin in stationary regime is modeled by a
one-dimensional Sturm-Liouville equation whose coefficients strongly depend on
its geometrical features. We are interested in the following issue: is there
any optimal shape maximizing the heat flux at the inlet of the fin? Two
relevant constraints are examined, by imposing either its volume or its
surface, and analytical nonexistence results are proved for both problems.
Furthermore, using specific perturbations, we explicitly compute the optimal
values and construct maximizing sequences. We show in particular that the
optimal heat flux at the inlet is infinite in the first case and finite in the
second one. Finally, we provide several extensions of these results for more
general models of heat conduction, as well as several numerical illustrations
Two-parameter Sturm-Liouville problems
This paper deals with the computation of the eigenvalues of two-parameter
Sturm- Liouville (SL) problems using the Regularized Sampling Method, a method
which has been effective in computing the eigenvalues of broad classes of SL
problems (Singular, Non-Self-Adjoint, Non-Local, Impulsive,...). We have shown,
in this work that it can tackle two-parameter SL problems with equal ease. An
example was provided to illustrate the effectiveness of the method.Comment: 9 page
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