Abstract
In our approach Schwartz distributions are defined as continuous linear functionals on an appropriate test function space. Thus this chapter starts with a reminder of some basic facts about the topological dual of an Hausdorff locally convex topological vector space. Then we proceed to define (general) Schwartz distributions T as continuous linear functionals on \(\mathcal{D}(\Omega)\), i.e., as an element of the topological dual \(\mathcal{D}^{\prime}(\Omega)\) of \(\mathcal{D}(\Omega)\). Similarly tempered distributions are defined as elements of the topological dual \(\mathcal{S}^{\prime}(\Omega)\) of the space \(\mathcal{S}(\Omega)\). Finally compactly supported distributions are elements of the topological dual \(\mathcal{E}^{\prime}(\Omega)\) of \(\mathcal{E}(\Omega)\). Furthermore regular distributions are introduced as the embedding of the space of locally integrable functions \(L^1_{loc}(\Omega)\) on Ω into \(\mathcal{D}^{\prime}(\Omega)\). Standard examples of distributions illustrate these definitions. When the distribution space \(\mathcal{D}^{\prime}(\Omega)\) is equipped with the weak topology \(\sigma=\sigma(\mathcal{D}^{\prime}(\Omega),\mathcal{D}(\Omega))\) it is sequentially complete. Localization of distributions is defined through the localized test functions in \(\mathcal{D}(\Omega)\). The resulting concept of support of a distribution is compatible with the notion of support of functions in \(L^1_{loc}(\Omega)\) through the standard embedding.
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© 2015 Springer International Publishing Switzerland
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Blanchard, P., Brüning, E. (2015). Schwartz Distributions. In: Mathematical Methods in Physics. Progress in Mathematical Physics, vol 69. Birkhäuser, Cham. https://doi.org/10.1007/978-3-319-14045-2_3
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DOI: https://doi.org/10.1007/978-3-319-14045-2_3
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Publisher Name: Birkhäuser, Cham
Print ISBN: 978-3-319-14044-5
Online ISBN: 978-3-319-14045-2
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