mathematical methods for physics iii (hilbert spaces)

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2013/2014 (2 nd semester) Mathematical Methods for Physics III 1 Mathematical Methods for Physics III (Hilbert Spaces) Lecturer: José Santiago: Theory and exercises (jsantiago @ugr.es) Office hours: M y J (11:00-13:00 y 14:00-15:00) office A03. Info on the course: www.ugr.es/~jsantiago/Docencia/MMIIIen/

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Page 1: Mathematical Methods for Physics III (Hilbert Spaces)

2013/2014 (2nd semester) Mathematical Methods for Physics III 1

Mathematical Methods for Physics III (Hilbert Spaces)

● Lecturer:● José Santiago: Theory and exercises (jsantiago

@ugr.es)– Office hours: M y J (11:00-13:00 y 14:00-15:00) office A03.

● Info on the course:– www.ugr.es/~jsantiago/Docencia/MMIIIen/

Page 2: Mathematical Methods for Physics III (Hilbert Spaces)

2013/2014 (2nd semester) Mathematical Methods for Physics III 2

Mathematical Methods for Physics III (Hilbert Spaces)

● Main Literature:– G. Helmberg, Introduction to spectral theory in Hilbert space, Dover,

1997.

– P. Roman, Some modern mathematics for physicists and other outsiders, vol. 2, Pergamon, 1975.

– P. Lax, Functional Analysis, Wiley 2002.

– L. Abellanas y A. Galindo, Espacios de Hilbert, Eudema, 1987.

– A. Vera López y P. Alegría Ezquerra, Un curso de Análisis Funcional. Teoría y problemas, AVL, 1997.

– A. Galindo y P. Pascual, Mecánica Cuántica, Eudema, 1989.

– E. Romera et al, Métodos Matemáticos, Paraninfo, 2013.

● Lecture notes are very succinct: examples, proofs and relevant comments on the blackboard (take your own notes)

Page 3: Mathematical Methods for Physics III (Hilbert Spaces)

2013/2014 (2nd semester) Mathematical Methods for Physics III 3

Motivation

● Postulates of Quantum Mechanics

● But not only QM, also differential and integral equations, ...

Every physical system is associated to a complex separable hilbert space and every pure state is described by a ray in such space

1st Postulate:

Every observable in a system is associated to a self-adjoint linear operator in the hilbert space whose eigenvalues are the possible outcomes of a measure of the observable

2nd Postulate:

The probability of getting a value ( ) when measuring an obserbable (A) in a pure state ( ) is , where is the projector on the eigenvalue proper subspace

3rd Postulate:

Page 4: Mathematical Methods for Physics III (Hilbert Spaces)

2013/2014 (2nd semester) Mathematical Methods for Physics III 4

Motivation

● But not only QM, also differential and integral equations, ...

● More generally, Hilbert Spaces are the mathematical structure needed to generalize (or ), including its geometrical features and operations with vectors to infinite dimensional vector spaces

Page 5: Mathematical Methods for Physics III (Hilbert Spaces)

2013/2014 (2nd semester) Mathematical Methods for Physics III 5

Outline

● Linear and metric spaces

● Normed and Banach spaces

● Spaces with scalar product and Hilbert spaces

● Spaces of functions. Eigenvector expansions

● Functionals and dual space. Distribution theory

● Operators in Hilbert Spaces

● Spectral theory

Page 6: Mathematical Methods for Physics III (Hilbert Spaces)

2013/2014 (2nd semester) Mathematical Methods for Physics III 6

Why Hilbert Spaces?

● They generalize the properties of to spaces of infinite dimension

LinearSpace

● (Finite) linear combinations of vectors. Linear independence. Linear basis.

MetricSpace

● Infinite linear combinations require limits: notion of distance

NormedSpace

● Translational invariant distance: it is enough with distance to the origin (norm)

(pre)HilbertSpace

● Generalization of : we need geometry (ortogonality, angles). Scalar product

Page 7: Mathematical Methods for Physics III (Hilbert Spaces)

2013/2014 (2nd semester) Mathematical Methods for Physics III 7

Linear Space

● Definition: Liear (or vector) space over a field Λ is a triad (L, +, .) formed by a non-empty set L and two binary operations (addition and scalar multiplication) that satisfy:

Page 8: Mathematical Methods for Physics III (Hilbert Spaces)

2013/2014 (2nd semester) Mathematical Methods for Physics III 8

Linear Space

● Trivial properties:

● Notation:

Page 9: Mathematical Methods for Physics III (Hilbert Spaces)

2013/2014 (2nd semester) Mathematical Methods for Physics III 9

Linear Space

● Definition: Linear subspace. Non-trivial subset of a linear space with the structure of a linear space.

● Properties:

● Definition. Linear span:

● Properties:

Page 10: Mathematical Methods for Physics III (Hilbert Spaces)

2013/2014 (2nd semester) Mathematical Methods for Physics III 10

Linear Space

● Definition: Linear independence.

● Definition: Hamel (or linear) basis. Maximal l.i. set (i.e. that it is not contained in any other l.i. set).

● Properties:

Page 11: Mathematical Methods for Physics III (Hilbert Spaces)

2013/2014 (2nd semester) Mathematical Methods for Physics III 11

Linear Space

● Definition: Subspace direct sum. Let be subsps. of L

● Theorem: Let L=M1+M2

● More generally, if L=M1+...+Mn

Page 12: Mathematical Methods for Physics III (Hilbert Spaces)

2013/2014 (2nd semester) Mathematical Methods for Physics III 12

Linear Space

● Summary:

● Linear (sub)space: (L,+,.)

● Linear span: [S]={FINITE linear combinations of elements of S}

● Linear independence: finite linear combination=0 al coeffs=0

● Hamel basis: Maximal l.i. set. Unique cardinal (linear dimension). Unique linear expansion of elements of L in terms of elements of B.

● Directa sum of subspaces: sum of subspaces with null intersection (to the sum of the remaining subspaces).

● Other results and definitions (mappings, inverse mapping, isomorphisms, projectors, …) can be defined here but we will postpone it to Hilbert spaces

Page 13: Mathematical Methods for Physics III (Hilbert Spaces)

2013/2014 (2nd semester) Mathematical Methods for Physics III 13

Metric spaces

● Definition: Metric space is a pair (X,d) where X is an arbitrary but non-empty set and is a function (distance or metric) that satisfies:

● Properties

Page 14: Mathematical Methods for Physics III (Hilbert Spaces)

2013/2014 (2nd semester) Mathematical Methods for Physics III 14

Metric spaces

● Definitions: Let (X,d) be a metric space.

● Open ball of radius r centered at x:

● Closed ball of radius r centered at x:

● Interior of A:

● Closure of A:

● Closed subspace:

● Dense subspace:

Page 15: Mathematical Methods for Physics III (Hilbert Spaces)

2013/2014 (2nd semester) Mathematical Methods for Physics III 15

Metric spaces

● Properties of open and closed subspaces:

Page 16: Mathematical Methods for Physics III (Hilbert Spaces)

2013/2014 (2nd semester) Mathematical Methods for Physics III 16

Metric spaces

● Definition: Convergent sequence

● Definition: Cauchy sequence

● Property: Every convergent sequence is a Cauchy sequence

● Definition: A metric space is complete if every Cauchy sequence is convergent. A subspace is complete if every Cauchy sequence in S converges in S

● Properties: Let

Page 17: Mathematical Methods for Physics III (Hilbert Spaces)

2013/2014 (2nd semester) Mathematical Methods for Physics III 17

Metric spaces

● Summary:

● Metric (sub)space: (X,d)

● Open and closed balls

● Interior point: open ball centered in x inside A

● int A= set of all interior points of A. Open subspace.

● Adherence point of A, every open ball centered in x has non-zero intersection with A. Closure of A. Closed subspace. Dense subspace in X

● Convergent sequence

● Cauchy sequence

● Complete metric space: Cauchy convergent

● Other properties (maps, continuity, boundedness, …) can be defined here but we will do it in Hilbert spaces.

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Normed spaces

● Definition: Normed space is a pair (X,||.||) where X is a linear space and is a function (norm) with the following properties:

● Every linear subspace of a normed space X is a normed subspace with the norm of X.

● Relation between normed and metric spaces

● Every nomed space is a metric space with the distance d(x,y)=||x-y||

● The associated distance satisfies

● Every metric linear space with these properties is a normed space with ||x||=d(x,0)

● Definition: Banach space. Complete normed space.

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2013/2014 (2nd semester) Mathematical Methods for Physics III 19

Normed spaces

● Properties:

● Completion theorem:

● Every normed linear space admits a completion , Banach space, unique up to norm isomorphisms, such that is dense in and

● Inifinite sums in normed spaces

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Normed spaces

● Hölder inequality (for sums):

● Minkowski inequality (for sums):

Page 21: Mathematical Methods for Physics III (Hilbert Spaces)

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Normed spaces

● Summary:

● Normed (sub)space: (X,||.||)

● Relation norm distance

● Banach space (complete normed space)

● Absolute convengence convergence in Banach spaces

● A subspace of a Banach space is Banach it is closed

● Completion theorem: every normed space can be made complete in a unique way

● An infinite sum converges in (X,||.||) to v if the sequence of partial sums converges to v

● Hölder and Minkowski inequalities

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Hilbert Space

● Definition: A pre-Hilbert space is a linear space with an associated scalar product.

● Scalar product: with the following properties

● In particular we have

Page 23: Mathematical Methods for Physics III (Hilbert Spaces)

2013/2014 (2nd semester) Mathematical Methods for Physics III 23

Hilbert Space

● Property: A pre-Hilbert space is a normed space with the norm associated to the scalar product

● Definition: A Hilbert space is a pre-Hilbert space that is complete with the norm associated to the scalar product (rather the distance associated to the norm).

● Properties: Let be a pre-Hilbert space and the associated norm:

● Relation between scalar product and norm: a normed space that satisfies the parallelogram identity is a pre-Hilbert space with a scalar product that satisfies

Page 24: Mathematical Methods for Physics III (Hilbert Spaces)

2013/2014 (2nd semester) Mathematical Methods for Physics III 24

Hilbert Space

● Properties: Let be a pre-Hilbert space and the associated norm:

● Schwarz-Cauchy-Buniakowski inequality

● Triangle inequality

● Continuity of the scalar product

Page 25: Mathematical Methods for Physics III (Hilbert Spaces)

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Hilbert Space

● Properties: Let be a pre-Hilbert space and the associated norm:

● (Generalized) Pythagora's Theorem:

● Pythagora's theorem

Page 26: Mathematical Methods for Physics III (Hilbert Spaces)

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Hilbert Space

● Properties:

● Finite Bessel inequality:

● Infinite Bessel inequality:

● Completion Theorem:

Page 27: Mathematical Methods for Physics III (Hilbert Spaces)

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Hilbert Space

● Definition: orthogonal complement

● Properties of the orthogonal complement

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Hilbert Space

● Theorem of orthogonal projection

Equivalent:

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Hilbert Space

● Properties:

● Definition: Orthogonal direct sum

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Hilbert Space

● Theorem:

● Theorem:

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Hilbert Space

● Orthonormalization theorem: Gram-Schmidt method

Solution:

● Definition: Orthonormal basis

● Theorem: Existence of orthonormal basis

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Hilbert Space

● Theorem: Characterization of orthonormal basis:

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Hilbert Space

● Definition: Separable topologial (and metric) space:

● A topological space X is separable if it contains a numerable subset dense in X.

● A metric space M is separable if and only if it has a numerable basis of open subsets.

● Separability criterion in Hilbert spaces

● Proposition:

● All orthonormal basis of a Hilbert space H have the same cardinal (Hilbert dimension of H).

Page 34: Mathematical Methods for Physics III (Hilbert Spaces)

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Hilbert Space

● Theorem of Hilbert Space classification

Definition:

Theorem:

Corolaries:

Page 35: Mathematical Methods for Physics III (Hilbert Spaces)

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Hilbert Space

● Summary:

● (Pre-)Hilbert space: Complete linear space with scalar product

● Hilbert Normed

● Parallelogram and polarization identities

● Schwarz and triangle inequality, continuity of scalar product

● Orthonormality. Pythagora's theorem and Bessel inequality

● Completion theorem

● Orthogonal complement and orthogonal projector. Best approximation to a vector.

● Gram-Schmidt orthonormalization method

● Orthonormal basis. Separable space

● Theorem of Hilbert Space classification

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Space of functions

● Some of the most important Hilbert spaces are spaces of functions.

● Examples:

● Example of not completeness of

● We can enlarge the space with the limits of all Cauchy sequences to complete it. We need a new concept of integral for that.

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Space of functions

● Riemann integral:

● Partition of the “x axis” and common convergence of upper and lower integrals

● Lebesgue integral:

● Partition of the “y axis” and measure of subsets of the “x axis”

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Space of functions

● We need a new concept of “measure”

● Borel set:

● Borel-Lebesgue measure (of a borel set B):

– Properties:

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Space of functions

● We need a new concept of “measure”

● Borel measurable function:

● f complex is Borel if both its real and imaginary parts are

● Characterization of Borel measurable functions:

● Lebesgue integral

Easy to extend to more general functions

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Space of functions

● Lebesgue integrable functions

● Properties almost everywhere (a.e.).

● L1 Spaces.

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Space of functions

● Lp spaces:

● Properties:

● Definition:

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Space of functions

● (Integral) Hölder and Minkowski inequalities

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Space of functions

● Some relevant orthonormal bases in L2:

● Legendre's basis

● Hermite's basis

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Space of functions

● Some relevant orthonormal bases in L2:

● Laguerre's basis

● Orthonormal bases of polynomial associated to a weight function

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Space of functions

● Some relevant orthonormal bases in L2:

● Fourier's basis

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Space of functions

● Some relevant orthonormal bases in L2:

● Fourier's basis

● Jordan convergence criterion

● Bases with only sines or cosines

Page 47: Mathematical Methods for Physics III (Hilbert Spaces)

2013/2014 (2nd semester) Mathematical Methods for Physics III 47

Space of functions

● Expansion in eigenvectors

● Consider the following differential operator

every function can be expanded in eigen-functions of

with

Eigenvalues

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● Summary:

● Borel sets. Borel-Lebesgue measure. Borel measurable functions.

● Lebesgue integral.

● Lebesgue integrable functions. Spaces

● Properties almost everywhere. Spaces

● is a Hilbert space (completion of )

● Hölder and Minkowski integral inequalities

● Orthonormal polynomials in

● Fourier basis. Fourier expansion.

● Expansion in eigenvectors.

Space of functions

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Linear forms

● Definitions:

● Theorem: Let F be a linear form in a normed space

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Linear forms

● Definition: Dual space of a Hilbert space (H,<,>) is the set of all continuous functional forms in H.

It is a Hilbert space (as we will see)

● Proposition: Let (H,<,>) be a Hilbert space of finite dimension:

● All functionals in H are continuous

● Riesz-Fréchet representation theorem: Let (H,<,>) be a Hilbert space (separable or not)

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Linear forms

● Properties:

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Linear forms

● Bilinear forms:

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Linear forms

● Strong convergence (in norm)

● Weak convergence

● Theorems:

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Distributions

● Test function spaces:

● Test functions of compact support

– Convergence

● Test functions of rapid decrease

– Convergence

● Properties

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Distributions

● Definitions and properties:

● Distribution:

● Space of distributions:

● Sufficient condition for T to be continuous

● Tempered distribution:

● Space of tempered distributions:

● The sufficient condition for continuity applies the same.

● Property:

Page 56: Mathematical Methods for Physics III (Hilbert Spaces)

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Distributions

● Operations with distributions

● Multiplication by a function:

● Derivative of a distribution:

● Shift:

● These operations are continuous with respect to the following definition of convercend of distributions

With this notion of convergence and are complete and is dense en

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Distributions

● Examples of distributions:

● Dirac's delta

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Distributions

● Examples of distributions:

● Principal value of (tempered distribution)

● Characteristic distribution (distribution)

1x

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Distributions

● Regularity theorem

● Fourier transform

● Fourier transform of distributions

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Linear forms and distributions

● Summary:

● Linear forms , bounded and continuous

● Dual space: bounded linear forms

● Riesz-Fréchet theorem: representation of linear forms in Hilbert spaces

● Bilinear forms and their representation in Hilbert spaces

● Spaces of test functions (bounded support and rapid decrease)

● (Tempered) distribution: linear form in spaces of test functions

● Operations with distributions: multiplication by a function, derivative, shift

● Examples of distributions: delta, step, PV(1/x), characteristic distribution

● Regularity theorem

● Fourier transform (of distributions).

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Operators in Hilbert spaces

● Definition:

● Properties:

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Operators in Hilbert spaces

● Definition:

● Definición:

● Theorem:

● Dual space:

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Operators in Hilbert spaces

● Property:

● Definition:

● Theorem (extension of operators bounded in a dense domain):

soluction

● Properties:

Page 64: Mathematical Methods for Physics III (Hilbert Spaces)

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Operators in Hilbert spaces

● Definition:

● Criterion of existence of the inverse operator

Note:

● Theorem (criterion of inversion with boundedness):

● Corolary:

Page 65: Mathematical Methods for Physics III (Hilbert Spaces)

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Operators in Hilbert spaces

● Topologies en :

● Uniform (or norm) topology

● Strong topology

● Weak topology

● In finite dimension (dim of H is finite) they are all equivalent

● In infinite dimension

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Operators in Hilbert spaces

● Some interesting operators

● Operators in finite dimension

● Destruction, creation and number operators (in )

● Rotation operador (in ).

● Shift operator (in ).

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Operators in Hilbert spaces

● Some interesting operators

● Position operador (en ).

● Derivative operador.

● Properties: let us define the position and momentum operators in

we have

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Operators in Hilbert spaces

● Adjoint operador

● Properties:

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Operators in Hilbert spaces

● Equality of operators

● Some special types of operators:

● Symmetric or hermitian operator

● Self-adjoint operator

● Bounded self-adjoint operator

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Operators in Hilbert spaces

● Properties of bounded self-adjoint operators

● Isometric operator

property

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Operators in Hilbert spaces

● Unitary operator

● Characterization of a unitary operator.

Note:

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Operators in Hilbert spaces

● Normal operator

● Properties:

Note:

● Orthogonal projector

● Theorem:

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Operators in Hilbert spaces

● Summary

● Operator , bounded and bounded in its domain

● Continuos operador bounded

● Theorem of extension of bounded operators with a dense domain

● Inverse operator. Existence of inverse operator (with boundedness)

● Uniform, strong and weak topologies in

● Examples of operators (finite dim., creation, destruction, number, position, derivative)

● Adjoint operator

● Hermitian, self-adjoin, isometric, unitary, normal operator

● Orthogonal projector

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Spectral theory

● Definition: Spectrum and resolvent of linear operators

● can be split in the following subsets, depending on the behavior of the operator

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Spectral theory

● Properties:

● Eigenvectors and eigenvalues

● Linear independence of eigenvectors with different eigenvalues

● Topological properties of the spectrum and resolvent

● Spectrum of the adjoint operator:

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Spectral theory

● Properties:

● Spectrum of normal operators:

● Spectrum of unitary operators (are normal):

● Spectrum of isometric operators (not normal in general):

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Spectral theory

● Properties:

● Spectrum of orthogonal projectors:

● Spectrum of self-adjoint operators:

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Spectral theory

● Definition:

● Theorem: