Spectral Geometry of Graphs.
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Superior document: | Operator Theory: Advances and Applications Series ; v.293 |
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Place / Publishing House: | Berlin, Heidelberg : : Springer Basel AG,, 2023. ©2024. |
Year of Publication: | 2023 |
Edition: | 1st ed. |
Language: | English |
Series: | Operator Theory: Advances and Applications Series
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Online Access: | |
Physical Description: | 1 online resource (644 pages) |
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Table of Contents:
- Intro
- Notations
- Conventions
- Contents
- 1 Very Personal Introduction
- 2 How to Define Differential Operators on Metric Graphs
- 2.1 Schrödinger Operators on Metric Graphs
- 2.1.1 Metric Graphs
- 2.1.2 Differential Operators
- 2.1.3 Standard Vertex Conditions
- 2.1.4 Definition of the Operator
- 2.2 Elementary Examples
- 3 Vertex Conditions
- 3.1 Preliminary Discussion
- 3.2 Vertex Conditions for the Star Graph
- 3.3 Vertex Conditions Via the Vertex Scattering Matrix
- 3.3.1 The Vertex Scattering Matrix
- 3.3.2 Scattering Matrix as a Parameterin the Vertex Conditions
- 3.3.3 On Properly Connecting Vertex Conditions
- 3.4 Parametrisation Via Hermitian Matrices
- 3.5 Scaling-Invariant and Standard Conditions
- 3.5.1 Energy Dependence of the Vertex S-matrix
- 3.5.2 Scaling-Invariant, or Non-Robin Vertex Conditions
- 3.5.3 Standard Vertex Conditions
- 3.6 Signing Conditions for Degree Two Vertices
- 3.7 Generalised Delta Couplings
- 3.8 Vertex Conditions for Arbitrary Graphs and Definition of the Magnetic Schrödinger Operator
- 3.8.1 Scattering Matrix Parametrisationof Vertex Conditions
- 3.8.2 Quadratic Form Parametrisation of Vertex Conditions
- Appendix 1: Important Classes of Vertex Conditions
- δ and δ'-Couplings
- Circulant Conditions
- `Real' Conditions
- Indistinguishable Edges
- Equi-transmitting Vertices
- Appendix 2: Parametrisation of Vertex Conditions: Historical Remarks
- Parametrisation Via Linear Relations
- Parametrisation Using Hermitian Operators
- Unitary Matrix Parametrisation
- 4 Elementary Spectral Properties of Quantum Graphs
- 4.1 Quantum Graphs as Self-adjoint Operators
- 4.2 The Dirichlet Operator and the Weyl's Law
- 4.3 Spectra of Quantum Graphs
- 4.4 Laplacian Ground State
- 4.5 Bonus Section: Positivity of the Ground Statefor Quantum Graphs.
- 4.5.1 The Case of Standard Vertex Conditions
- 4.5.2 A Counterexample
- 4.5.3 Invariance of the Quadratic Form
- 4.5.4 Positivity of the Ground State for Generalised Delta-Couplings
- 4.6 First Spectral Estimates
- 5 The Characteristic Equation
- 5.1 Characteristic Equation I: Edge Transfer Matrices
- 5.1.1 Transfer Matrix for a Single Interval
- One-Dimensional Schrödinger Equation
- Magnetic Schrödinger Equation
- 5.1.2 The Characteristic Equation
- 5.1.3 The Characteristic Equation, Second Look
- 5.2 Characteristic Equation II: Scattering Approach
- 5.2.1 On the Scattering Matrix Associated with a Compact Interval
- 5.2.2 Positive Spectrum and Scattering Matrices for Finite Compact Graphs
- 5.3 Characteristic Equation III: M-Function Approach
- 5.3.1 M-Function for a Single Interval
- 5.3.2 The Edge M-Function
- 5.3.3 Characteristic Equation via the M-Function: General Vertex Conditions
- 5.3.4 Reduction of the M-Function for Standard Vertex Conditions
- 6 Standard Laplacians and Secular Polynomials
- 6.1 Secular Polynomials
- 6.2 Secular Polynomials for Small Graphs
- 6.3 Zero Sets for Small Graphs
- Appendix 1: Singular Sets on Secular Manifolds, Proof of Lemma 6.3
- 7 Reducibility of Secular Polynomials
- 7.1 Contraction of Graphs
- 7.2 Extensions of Graphs
- 7.3 Secular Polynomials for the Watermelon Graphand Its Closest Relatives
- 7.4 Secular Polynomials for Flower Graphs and Their Extensions
- 7.5 Reducibility of Secular Polynomials for General Graphs
- 8 The Trace Formula
- 8.1 The Characteristic Equation: Multiplicityof Positive Eigenvalues
- 8.2 Algebraic and Spectral Multiplicities of the Eigenvalue Zero
- 8.3 The Trace Formula for Standard Laplacians
- 8.4 Trace Formula for Laplacians with Scaling-InvariantVertex Conditions
- 9 Trace Formula and Inverse Problems.
- 9.1 Euler Characteristic for Standard Laplacians
- 9.2 Euler Characteristic for Graphs with Dirichlet Vertices
- 9.3 Spectral Asymptotics and Schrödinger Operators
- 9.3.1 Euler Characteristic and Spectral Asymptotics
- 9.3.2 Schrödinger Operators and Euler Characteristic of Graphs
- 9.3.3 General Vertex Conditions: A Counterexample
- 9.4 Reconstruction of Graphs with RationallyIndependent Lengths
- 10 Arithmetic Structure of the Spectrumand Crystalline Measures
- 10.1 Arithmetic Structure of the Spectrum
- 10.2 Crystalline Measures
- 10.3 The Lasso Graph and Crystalline Measures
- 10.4 Graph's Spectrum as a Delone Set
- 11 Quadratic Forms and Spectral Estimates
- 11.1 Quadratic Forms (Integrable Potentials)
- 11.1.1 Explicit Expression
- 11.1.2 An Elementary Sobolev Estimate
- 11.1.3 The Perturbation Term Is Form-Bounded
- 11.1.4 The Reference Laplacian
- 11.1.5 Closure of the Perturbed Quadratic Form
- 11.2 Spectral Estimates (Standard Vertex Conditions)
- 11.3 Spectral Estimates for General Vertex Conditions
- 12 Spectral Gap and Dirichlet Ground State
- 12.1 Fundamental Estimates
- 12.1.1 Eulerian Path Technique
- 12.1.2 Symmetrisation Technique
- 12.2 Balanced and Doubly Connected Graphs
- 12.3 Graphs with Dirichlet Vertices
- 12.4 Cheeger's Approach
- 12.5 Topological Perturbations in the Case of Standard Conditions
- 12.5.1 Gluing Vertices Together
- 12.5.2 Adding an Edge
- 12.6 Bonus Section: Further Topological Perturbations
- 12.6.1 Cutting Edges
- 12.6.2 Deleting Edges
- 13 Higher Eigenvalues and Topological Perturbations
- 13.1 Fundamental Estimates for Higher Eigenvalues
- 13.1.1 Lower Estimates
- 13.1.2 Upper Bounds
- 13.1.3 Graphs Realising Extremal Eigenvalues
- 13.2 Gluing and Cutting Vertices with Standard Conditions
- 13.3 Gluing Vertices with Scaling-Invariant Conditions.
- 13.3.1 Scaling-Invariant Conditions Revisited
- 13.3.2 Gluing Vertices
- Gluing Vertices with One-Dimensional Vertex Conditions
- Gluing Vertices with Hyperplanar Vertex Conditions
- 13.3.3 Spectral Gap and Gluing Vertices with Scaling-Invariant Conditions
- 13.4 Gluing Vertices with General Vertex Conditions
- 14 Ambartsumian Type Theorems
- 14.1 Two Parameters Fixed, One Parameter Varies
- 14.1.1 Zero Potential Is Exceptional: Classical Ambartsumian Theorem
- 14.1.2 Interval-Graph Is Exceptional: Geometric Version of Ambartsumian Theorem for Standard Laplacians
- 14.1.3 Standard Vertex Conditions Are Not Exceptional
- 14.2 One Parameter Is Fixed, Two Parameters Vary
- 14.2.1 Standard Vertex Conditions Are Exceptional: Schrödinger Operators on Arbitrary Graphs
- 14.2.2 Zero Potential: Laplacians on Graphs that Are Isospectral to the Interval
- 14.2.3 Single Interval: Schrödinger Operators Isospectral to the Standard Laplacian
- Crum's Procedure
- Inverting Crum's Procedure
- 15 Further Theorems Inspired by Ambartsumian
- 15.1 Ambartsumian-Type Theorem by Davies
- 15.1.1 On a Sufficient Condition for the Potential to Be Zero
- 15.1.2 Laplacian Heat Kernel
- Heat Kernel for the Dirichlet Laplacian on an Interval
- Heat Kernel for the Standard Laplacian on the Graph
- 15.1.3 On Schrödinger Semigroups
- 15.1.4 A Theorem by Davies
- 15.2 On Asymptotically Isospectral Quantum Graphs
- 15.2.1 On the Zeroes of Generalised TrigonometricPolynomials
- 15.2.2 Asymptotically Isospectral Quantum Graphs
- 15.2.3 When a Schrödinger Operator Is Isospectral to a Laplacian
- 16 Magnetic Fluxes
- 16.1 Unitary Transformations via Multiplications and Magnetic Schrödinger Operators
- 16.2 Vertex Phases and Transition Probabilities
- 16.3 Topological Damping of Aharonov-Bohm Effect
- 16.3.1 Getting Started.
- 16.3.2 Explicit Calculation of the Spectrum
- 16.3.3 Topological Reasons for Damping
- 17 M-Functions: Definitions and Examples
- 17.1 The Graph M-Function
- 17.1.1 Motivation and Historical Hints
- 17.1.2 The Formal Definition
- 17.1.3 Examples
- 17.2 Explicit Formulas Using Eigenfunctions
- 17.3 Hierarchy of M-Functions for Standard Vertex Conditions
- 18 M-Functions: Properties and First Applications
- 18.1 M-Function as a Matrix-Valued Herglotz-Nevanlinna Function
- 18.2 Gluing Procedure and the Spectral Gap
- 18.2.1 Examples
- 18.3 Gluing Graphs and M-Functions
- 18.3.1 The M-Function for General Vertex Conditions at the Contact Set
- 18.3.2 Gluing Graphs with General Vertex Conditions
- Appendix 1: Scattering from Compact Graphs
- 19 Boundary Control: BC-Method
- 19.1 Inverse Problems: First Look
- 19.2 How to Use BC-Method for Graphs
- 19.3 The Response Operator and the M-Function
- 19.4 Inverse Problem for the One-DimensionalSchrödinger Equation
- 19.5 BC-Method for the Standard Laplacian on the Star Graph
- 19.6 BC-Method for the Star Graph with General Vertex Conditions
- 20 Inverse Problems for Trees
- 20.1 Obvious Ambiguities and Limitations
- 20.2 Subproblem I: Reconstruction of the Metric Tree
- 20.2.1 Global Reconstruction of the Metric Tree
- 20.2.2 Local Reconstruction of the Metric Tree
- 20.3 Subproblem II: Reconstruction of the Potential
- 20.4 Subproblem III: Reconstruction of the Vertex Conditions
- 20.4.1 Trimming a Bunch
- 20.4.2 Recovering the Vertex Conditions for an Equilateral Bunch
- 20.5 Cleaning and Pruning Using the M-functions
- 20.5.1 Cleaning the Edges
- 20.5.2 Pruning Branches and Bunches
- 20.6 Complete Solution of the Inverse Problem for Trees
- Appendix 1: Calculation of the M-function for the Cross Graph
- Appendix 2: Calderón Problem.
- 21 Boundary Control for Graphs with Cycles: Dismantling Graphs.