On closed non-vanishing ideals in CB(X) I; Connectedness properties
Introduction
Throughout this article by a space we mean a topological space. Completely regular spaces are assumed to be Hausdorff. The field of scalars, denoted by , is either or and is fixed throughout our discussion. For a space X we denote by the set of all bounded continuous scalar-valued mappings on X. The set is a Banach algebra when equipped with pointwise addition and multiplication and the supremum norm. We denote by the normed subalgebra of consisting of mappings which vanish at infinity.
The Banach algebra plays a fundamental role in both topology and analysis. Here we assume the minimal assumption of complete regularity on the space X, and concentrate on the study of closed ideals H of which are non-vanishing, in the sense that, there is no point of X at which every element of H vanishes. This is done by studying the (unique) locally compact Hausdorff space Y which is associated to H in such a way that H and are isometrically isomorphic. The space Y is constructed by the second author in [8] as a subspace of the Stone–Čech compactification of X, and coincides with the spectrum of H (considered as a Banach algebra) in the case when the field of scalars is . The known (and simple) structure of Y enables us to study its properties. We are particularly interested in connectedness properties of Y. More specifically, we find necessary and sufficient (algebraic) conditions for H such that Y satisfies (topological) properties such as locally connectedness, total disconnectedness, zero-dimensionality, strong zero-dimensionality, total separatedness or extremal disconnectedness.
Throughout this article we will make critical use of the theory of the Stone–Čech compactification. We state some basic properties of the Stone–Čech compactification in the following and refer the reader to the standard texts [4] and [11] for further reading on the subject.
The Stone–Čech compactification. Let X be completely regular space. By a compactification of X we mean a compact Hausdorff space αX which contains X as a dense subspace. Among compactifications of X there is the “largest” one called the Stone–Čech compactification (and denoted by βX) which is characterized by the property that every bounded continuous mapping is extendible to a continuous mapping . For a bounded continuous mapping we denote by or the (unique) continuous extension of f to βX.
The following are a few of the basic properties of βX. We use these properties throughout without explicitly referring to them.
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if .
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X is locally compact if and only if X is open in βX.
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is open-and-closed in βX if M is open-and-closed in X.
Section snippets
Preliminaries
In [8] (Section 3.2) the second author has studied closed non-vanishing ideals of , where X is a completely regular space, by relating them to certain subspaces of the Stone–Čech compactification of X. The precise statement is as follows. (See Theorem 3.9 of [8].)
Recall that for a mapping the cozeroset of f, denoted by , is the set of all y in Y such that .
Theorem and Notation 2.1 Let X be a completely regular space. Let H be a non-vanishing closed ideal in . Let We call
Local connectedness of the spectrum
In this section we provide a necessary and sufficient condition for the spectrum of a non-vanishing closed ideal of to be locally connected. (Recall that a space Y is called locally connected if every neighborhood of any point of Y contains a connected open neighborhood.) Here, as usual, X is a completely regular space and is endowed with pointwise addition and multiplication and the supremum norm. Our theorem is motivated by Theorem 3.2.12 of [8] (quoted here in the previous
Various connectedness properties of the spectrum
In this section we study various (dis)connectedness properties of the spectrum of a non-vanishing closed ideal of . (As usual, X is a completely regular space and is endowed with pointwise addition and multiplication and the supremum norm.) The properties under consideration are total disconnectedness, zero-dimensionality, strong zero-dimensionality, total separatedness and extremal disconnectedness.
Recall that a completely regular space Y is called
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totally disconnected if Y has no
Acknowledgements
The authors wish to thank the referee for reading the manuscript and for his/her comments.
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