In mathematics, the ba space [math]\displaystyle{ ba(\Sigma) }[/math] of an algebra of sets [math]\displaystyle{ \Sigma }[/math] is the Banach space consisting of all bounded and finitely additive signed measures on [math]\displaystyle{ \Sigma }[/math]. The norm is defined as the variation, that is [math]\displaystyle{ \|\nu\|=|\nu|(X). }[/math][1]
If Σ is a sigma-algebra, then the space [math]\displaystyle{ ca(\Sigma) }[/math] is defined as the subset of [math]\displaystyle{ ba(\Sigma) }[/math] consisting of countably additive measures.[2] The notation ba is a mnemonic for bounded additive and ca is short for countably additive.
If X is a topological space, and Σ is the sigma-algebra of Borel sets in X, then [math]\displaystyle{ rca(X) }[/math] is the subspace of [math]\displaystyle{ ca(\Sigma) }[/math] consisting of all regular Borel measures on X.[3]
All three spaces are complete (they are Banach spaces) with respect to the same norm defined by the total variation, and thus [math]\displaystyle{ ca(\Sigma) }[/math] is a closed subset of [math]\displaystyle{ ba(\Sigma) }[/math], and [math]\displaystyle{ rca(X) }[/math] is a closed set of [math]\displaystyle{ ca(\Sigma) }[/math] for Σ the algebra of Borel sets on X. The space of simple functions on [math]\displaystyle{ \Sigma }[/math] is dense in [math]\displaystyle{ ba(\Sigma) }[/math].
The ba space of the power set of the natural numbers, ba(2N), is often denoted as simply [math]\displaystyle{ ba }[/math] and is isomorphic to the dual space of the ℓ∞ space.
Let B(Σ) be the space of bounded Σ-measurable functions, equipped with the uniform norm. Then ba(Σ) = B(Σ)* is the continuous dual space of B(Σ). This is due to Hildebrandt[4] and Fichtenholtz & Kantorovich.[5] This is a kind of Riesz representation theorem which allows for a measure to be represented as a linear functional on measurable functions. In particular, this isomorphism allows one to define the integral with respect to a finitely additive measure (note that the usual Lebesgue integral requires countable additivity). This is due to Dunford & Schwartz,[6] and is often used to define the integral with respect to vector measures,[7] and especially vector-valued Radon measures.
The topological duality ba(Σ) = B(Σ)* is easy to see. There is an obvious algebraic duality between the vector space of all finitely additive measures σ on Σ and the vector space of simple functions ([math]\displaystyle{ \mu(A)=\zeta\left(1_A\right) }[/math]). It is easy to check that the linear form induced by σ is continuous in the sup-norm if σ is bounded, and the result follows since a linear form on the dense subspace of simple functions extends to an element of B(Σ)* if it is continuous in the sup-norm.
If Σ is a sigma-algebra and μ is a sigma-additive positive measure on Σ then the Lp space L∞(μ) endowed with the essential supremum norm is by definition the quotient space of B(Σ) by the closed subspace of bounded μ-null functions:
The dual Banach space L∞(μ)* is thus isomorphic to
i.e. the space of finitely additive signed measures on Σ that are absolutely continuous with respect to μ (μ-a.c. for short).
When the measure space is furthermore sigma-finite then L∞(μ) is in turn dual to L1(μ), which by the Radon–Nikodym theorem is identified with the set of all countably additive μ-a.c. measures. In other words, the inclusion in the bidual
is isomorphic to the inclusion of the space of countably additive μ-a.c. bounded measures inside the space of all finitely additive μ-a.c. bounded measures.
Original source: https://en.wikipedia.org/wiki/Ba space.
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