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Banach algebra

From Wikipedia, the free encyclopedia
(Redirected fromStructure space)
Particular kind of algebraic structure

Inmathematics, especiallyfunctional analysis, aBanach algebra, named afterStefan Banach, is anassociative algebraA{\displaystyle A} over thereal orcomplex numbers (or over anon-Archimedean completenormed field) that at the same time is also aBanach space, that is, anormed space that iscomplete in themetric induced by the norm. The norm is required to satisfyxy xy for all x,yA.{\displaystyle \|x\,y\|\ \leq \|x\|\,\|y\|\quad {\text{ for all }}x,y\in A.}

This ensures that the multiplication operation iscontinuous with respect to themetric topology.

A Banach algebra is calledunital if it has anidentity element for the multiplication whose norm is1,{\displaystyle 1,} andcommutative if its multiplication iscommutative.Any Banach algebraA{\displaystyle A} (whether it is unital or not) can be embeddedisometrically into a unital Banach algebraAe{\displaystyle A_{e}} so as to form aclosedideal ofAe{\displaystyle A_{e}}. Often one assumesa priori that the algebra under consideration is unital because one can develop much of the theory by consideringAe{\displaystyle A_{e}} and then applying the outcome in the original algebra. However, this is not the case all the time. For example, one cannot define all thetrigonometric functions in a Banach algebra without identity.

The theory of real Banach algebras can be very different from the theory of complex Banach algebras. For example, thespectrum of an element of a nontrivial complex Banach algebra can never be empty, whereas in a real Banach algebra it could be empty for some elements.

Banach algebras can also be defined over fields ofp{\displaystyle p}-adic numbers. This is part ofp{\displaystyle p}-adic analysis.

Examples

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The prototypical example of a Banach algebra isC0(X){\displaystyle C_{0}(X)}, the space of (complex-valued) continuous functions, defined on alocally compact Hausdorff spaceX{\displaystyle X}, thatvanish at infinity.C0(X){\displaystyle C_{0}(X)} is unital if and only ifX{\displaystyle X} iscompact. Thecomplex conjugation being aninvolution,C0(X){\displaystyle C_{0}(X)} is in fact aC*-algebra. More generally, every C*-algebra is a Banach algebra by definition.

Properties

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Severalelementary functions that are defined viapower series may be defined in any unital Banach algebra; examples include theexponential function and thetrigonometric functions, and more generally anyentire function. (In particular, the exponential map can be used to defineabstract index groups.) The formula for thegeometric series remains valid in general unital Banach algebras. Thebinomial theorem also holds for two commuting elements of a Banach algebra.

The set ofinvertible elements in any unital Banach algebra is anopen set, and the inversion operation on this set is continuous (and hence is a homeomorphism), so that it forms atopological group under multiplication.[3]

If a Banach algebra has unit1,{\displaystyle \mathbf {1} ,} then1{\displaystyle \mathbf {1} } cannot be acommutator; that is,xyyx1{\displaystyle xy-yx\neq \mathbf {1} } for anyx,yA.{\displaystyle x,y\in A.} This is becausexy{\displaystyle xy} andyx{\displaystyle yx} have the samespectrum except possibly0.{\displaystyle 0.}

The various algebras of functions given in the examples above have very different properties from standard examples of algebras such as the reals. For example:

Spectral theory

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Main article:Spectral theory

Unital Banach algebras over the complex field provide a general setting to develop spectral theory. Thespectrum of an elementxA,{\displaystyle x\in A,} denoted byσ(x){\displaystyle \sigma (x)}, consists of all those complexscalarsλ{\displaystyle \lambda } such thatxλ1{\displaystyle x-\lambda \mathbf {1} } is not invertible inA.{\displaystyle A.} The spectrum of any elementx{\displaystyle x} is a closed subset of the closed disc inC{\displaystyle \mathbb {C} } with radiusx{\displaystyle \|x\|} and center0,{\displaystyle 0,} and thus iscompact. Moreover, the spectrumσ(x){\displaystyle \sigma (x)} of an elementx{\displaystyle x} isnon-empty and satisfies thespectral radius formula:sup{|λ|:λσ(x)}=limnxn1/n.{\displaystyle \sup\{|\lambda |:\lambda \in \sigma (x)\}=\lim _{n\to \infty }\|x^{n}\|^{1/n}.}

GivenxA,{\displaystyle x\in A,} theholomorphic functional calculus allows to definef(x)A{\displaystyle f(x)\in A} for any functionf{\displaystyle f}holomorphic in a neighborhood ofσ(x).{\displaystyle \sigma (x).} Furthermore, the spectral mapping theorem holds:[5]σ(f(x))=f(σ(x)).{\displaystyle \sigma (f(x))=f(\sigma (x)).}

When the Banach algebraA{\displaystyle A} is the algebraL(X){\displaystyle L(X)} of bounded linear operators on a complex Banach spaceX{\displaystyle X} (for example, the algebra of square matrices), the notion of the spectrum inA{\displaystyle A} coincides with the usual one inoperator theory. ForfC(X){\displaystyle f\in C(X)} (with a compact Hausdorff spaceX{\displaystyle X}), one sees that:σ(f)={f(t):tX}.{\displaystyle \sigma (f)=\{f(t):t\in X\}.}

The norm of a normal elementx{\displaystyle x} of a C*-algebra coincides with its spectral radius. This generalizes an analogous fact for normal operators.

LetA{\displaystyle A} be a complex unital Banach algebra in which every non-zero elementx{\displaystyle x} is invertible (a division algebra). For everyaA,{\displaystyle a\in A,} there isλC{\displaystyle \lambda \in \mathbb {C} } such thataλ1{\displaystyle a-\lambda \mathbf {1} } is not invertible (because the spectrum ofa{\displaystyle a} is not empty) hencea=λ1:{\displaystyle a=\lambda \mathbf {1} :} this algebraA{\displaystyle A} is naturally isomorphic toC{\displaystyle \mathbb {C} } (the complex case of the Gelfand–Mazur theorem).

Ideals and characters

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LetA{\displaystyle A} be a unitalcommutative Banach algebra overC.{\displaystyle \mathbb {C} .} SinceA{\displaystyle A} is then a commutative ring with unit, every non-invertible element ofA{\displaystyle A} belongs to somemaximal ideal ofA.{\displaystyle A.} Since a maximal idealm{\displaystyle {\mathfrak {m}}} inA{\displaystyle A} is closed,A/m{\displaystyle A/{\mathfrak {m}}} is a Banach algebra that is a field, and it follows from theGelfand–Mazur theorem that there is a bijection between the set of all maximal ideals ofA{\displaystyle A} and the setΔ(A){\displaystyle \Delta (A)} of all nonzero homomorphisms fromA{\displaystyle A} toC.{\displaystyle \mathbb {C} .} The setΔ(A){\displaystyle \Delta (A)} is called thestructure space orcharacter space ofA{\displaystyle A}.

AcharacterχΔ(A){\displaystyle \chi \in \Delta (A)} is a linear functional onA{\displaystyle A} that is at the same time multiplicative,χ(ab)=χ(a)χ(b),{\displaystyle \chi (ab)=\chi (a)\chi (b),} and satisfiesχ(1)=1.{\displaystyle \chi (\mathbf {1} )=1.} Every character is automatically continuous fromA{\displaystyle A} toC,{\displaystyle \mathbb {C} ,} since the kernel of a character is a maximal ideal, which is closed. Moreover, the norm (that is, operator norm) of a character is one. Equipped with the topology of pointwise convergence onA{\displaystyle A} (that is, the topology induced by theweak-* topology ofA{\displaystyle A^{*}}), the character space,Δ(A),{\displaystyle \Delta (A),} is a compact Hausdorff space.

For anyxA,{\displaystyle x\in A,}σ(x)=σ(x^){\displaystyle \sigma (x)=\sigma ({\hat {x}})}wherex^{\displaystyle {\hat {x}}} is theGelfand representation ofx{\displaystyle x} defined as follows:x^{\displaystyle {\hat {x}}} is the continuous function fromΔ(A){\displaystyle \Delta (A)} toC{\displaystyle \mathbb {C} } given byx^(χ)=χ(x).{\displaystyle {\hat {x}}(\chi )=\chi (x).} The spectrum ofx^,{\displaystyle {\hat {x}},} in the formula above, is the spectrum as element of the algebraC(Δ(A)){\displaystyle C(\Delta (A))} of complex continuous functions on the compact spaceΔ(A).{\displaystyle \Delta (A).} Explicitly,σ(x^)={χ(x):χΔ(A)}.{\displaystyle \sigma ({\hat {x}})=\{\chi (x):\chi \in \Delta (A)\}.}

As an algebra, a unital commutative Banach algebra issemisimple (that is, itsJacobson radical is zero) if and only if its Gelfand representation has trivial kernel. An important example of such an algebra is a commutative C*-algebra. In fact, whenA{\displaystyle A} is a commutative unital C*-algebra, the Gelfand representation is then an isometric *-isomorphism betweenA{\displaystyle A} andC(Δ(A)).{\displaystyle C(\Delta (A)).}[a]

Banach *-algebras

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A Banach *-algebraA{\displaystyle A} is a Banach algebra over the field ofcomplex numbers, together with a map:AA{\displaystyle {}^{*}:A\to A} that has the following properties:

  1. (x)=x{\displaystyle \left(x^{*}\right)^{*}=x} for allxA{\displaystyle x\in A} (so the map is aninvolution).
  2. (x+y)=x+y{\displaystyle (x+y)^{*}=x^{*}+y^{*}} for allx,yA.{\displaystyle x,y\in A.}
  3. (λx)=λ¯x{\displaystyle (\lambda x)^{*}={\bar {\lambda }}x^{*}} for everyλC{\displaystyle \lambda \in \mathbb {C} } and everyxA;{\displaystyle x\in A;} here,λ¯{\displaystyle {\bar {\lambda }}} denotes thecomplex conjugate ofλ.{\displaystyle \lambda .}
  4. (xy)=yx{\displaystyle (xy)^{*}=y^{*}x^{*}} for allx,yA.{\displaystyle x,y\in A.}

In other words, a Banach *-algebra is a Banach algebra overC{\displaystyle \mathbb {C} } that is also a*-algebra.

In most natural examples, one also has that the involution isisometric, that is,x=x for all xA.{\displaystyle \|x^{*}\|=\|x\|\quad {\text{ for all }}x\in A.}Some authors include this isometric property in the definition of a Banach *-algebra.

A Banach *-algebra satisfyingxx=xx{\displaystyle \|x^{*}x\|=\|x^{*}\|\|x\|} is aC*-algebra.

See also

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Notes

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  1. ^Proof: Since every element of a commutative C*-algebra is normal, the Gelfand representation is isometric; in particular, it is injective and its image is closed. But the image of the Gelfand representation is dense by theStone–Weierstrass theorem.

Citations

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  1. ^Conway 1990, Example VII.1.8.
  2. ^abConway 1990, Example VII.1.9.
  3. ^Conway 1990, Theorem VII.2.2.
  4. ^García, Miguel Cabrera; Palacios, Angel Rodríguez (1995)."A New Simple Proof of the Gelfand-Mazur-Kaplansky Theorem".Proceedings of the American Mathematical Society.123 (9):2663–2666.doi:10.2307/2160559.ISSN 0002-9939.JSTOR 2160559.
  5. ^Takesaki 1979, Proposition 2.8.

References

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