Steklov operator
E910282
The Steklov operator is a boundary integral operator arising in the study of elliptic partial differential equations and spectral problems, particularly in the context of Steklov eigenvalue problems.
All labels observed (1)
| Label | Occurrences |
|---|---|
| Steklov operator canonical | 1 |
How this entity was disambiguated
This entity first appeared as the object of triple T11186005 — resolving that mention is where its identity was fixed. The disambiguator weighed these candidate entities and picked the highlighted one (or “None”, minting a new entity). This is how homonymy is resolved: the same surface form can point to different entities.
Target entity: Steklov operator Context triple: [Vladimir Steklov, hasEponym, Steklov operator]
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A.
Sturm–Liouville problem
The Sturm–Liouville problem is a class of second-order linear differential equations with boundary conditions that yield real eigenvalues and orthogonal eigenfunctions forming a basis for function expansions in mathematical physics and engineering.
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B.
Fredholm operator
A Fredholm operator is a bounded linear operator between Banach (or Hilbert) spaces with finite-dimensional kernel and cokernel and a closed range, characterized by its integer-valued index.
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C.
Hilbert–Schmidt operators
Hilbert–Schmidt operators are a class of compact operators on Hilbert spaces characterized by having finite Hilbert–Schmidt norm, playing a central role in functional analysis and operator theory.
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D.
Laplace operator
The Laplace operator is a second-order differential operator widely used in mathematics and physics to describe phenomena such as diffusion, heat flow, and wave propagation.
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E.
Jacobi operator
The Jacobi operator is a linear differential operator central to the theory of elliptic functions and integrable systems, named after the mathematician Carl Gustav Jacob Jacobi.
- F. None of above. chosen
- G. Unsure - the case is ambiguous/there is not enough information to decide.
Target entity: Steklov operator Target entity description: The Steklov operator is a boundary integral operator arising in the study of elliptic partial differential equations and spectral problems, particularly in the context of Steklov eigenvalue problems.
-
A.
Sturm–Liouville problem
The Sturm–Liouville problem is a class of second-order linear differential equations with boundary conditions that yield real eigenvalues and orthogonal eigenfunctions forming a basis for function expansions in mathematical physics and engineering.
-
B.
Fredholm operator
A Fredholm operator is a bounded linear operator between Banach (or Hilbert) spaces with finite-dimensional kernel and cokernel and a closed range, characterized by its integer-valued index.
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C.
Hilbert–Schmidt operators
Hilbert–Schmidt operators are a class of compact operators on Hilbert spaces characterized by having finite Hilbert–Schmidt norm, playing a central role in functional analysis and operator theory.
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D.
Laplace operator
The Laplace operator is a second-order differential operator widely used in mathematics and physics to describe phenomena such as diffusion, heat flow, and wave propagation.
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E.
Jacobi operator
The Jacobi operator is a linear differential operator central to the theory of elliptic functions and integrable systems, named after the mathematician Carl Gustav Jacob Jacobi.
- F. None of above. chosen
Statements (46)
| Predicate | Object |
|---|---|
| instanceOf |
boundary integral operator
ⓘ
linear operator ⓘ mathematical operator ⓘ |
| actsOn | functions on the boundary of a domain ⓘ |
| alsoCalled | Dirichlet-to-Neumann map NERFINISHED ⓘ |
| appearsIn | Calderón inverse conductivity problem NERFINISHED ⓘ |
| arisesIn |
Steklov eigenvalue problems
NERFINISHED
ⓘ
boundary value problems ⓘ elliptic partial differential equations ⓘ |
| associatedWith |
Laplace equation
NERFINISHED
ⓘ
Steklov boundary conditions NERFINISHED ⓘ harmonic functions ⓘ |
| classification | non-local boundary operator ⓘ |
| context |
Riemannian manifolds with boundary
ⓘ
bounded domains in Euclidean space ⓘ |
| dependsOn |
geometry of the domain
ⓘ
metric on the boundary ⓘ |
| domain | boundary of a domain ⓘ |
| eigenvalueProblem |
Steklov eigenfunctions
NERFINISHED
ⓘ
Steklov spectrum NERFINISHED ⓘ |
| field |
mathematical analysis
ⓘ
partial differential equations ⓘ spectral theory ⓘ |
| generalizationOf | classical Steklov boundary condition operator ⓘ |
| hasKernel | constant functions on the boundary (in many standard settings) ⓘ |
| hasProperty |
elliptic pseudodifferential operator of order 1 (on smooth boundaries)
ⓘ
positive (under suitable conditions) ⓘ self-adjoint (under suitable conditions) ⓘ |
| isDefinedFor | solutions of elliptic PDEs in a domain ⓘ |
| maps | Dirichlet boundary data to Neumann boundary data ⓘ |
| mathematicalCategory | unbounded operator on a Hilbert space (in typical formulations) ⓘ |
| namedAfter | Vladimir Andreevich Steklov NERFINISHED ⓘ |
| namedFor | Steklov eigenvalue problem NERFINISHED ⓘ |
| relatedTo |
Calderón projector
NERFINISHED
ⓘ
Neumann-to-Dirichlet map NERFINISHED ⓘ boundary integral equations ⓘ |
| requires | elliptic regularity theory for definition and analysis ⓘ |
| spectralData |
Steklov eigenvalues accumulate only at infinity
ⓘ
Steklov eigenvalues form a discrete sequence under standard assumptions ⓘ |
| typicalHilbertSpace | L^2 of the boundary measure GENERATED ⓘ |
| usedIn |
control theory for PDEs
ⓘ
inverse problems ⓘ shape optimization ⓘ spectral geometry ⓘ |
| usedToStudy |
boundary determination problems
ⓘ
relationship between boundary geometry and spectrum ⓘ |
How these facts were elicited
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Subject: Steklov operator Description of subject: The Steklov operator is a boundary integral operator arising in the study of elliptic partial differential equations and spectral problems, particularly in the context of Steklov eigenvalue problems.
Referenced by (1)
Full triples — surface form annotated when it differs from this entity's canonical label.