35,557 research outputs found

    Eigenfunction expansions for a fundamental solution of Laplace's equation on R3\R^3 in parabolic and elliptic cylinder coordinates

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    A fundamental solution of Laplace's equation in three dimensions is expanded in harmonic functions that are separated in parabolic or elliptic cylinder coordinates. There are two expansions in each case which reduce to expansions of the Bessel functions J0(kr)J_0(kr) or K0(kr)K_0(kr), r2=(x−x0)2+(y−y0)2r^2=(x-x_0)^2+(y-y_0)^2, in parabolic and elliptic cylinder harmonics. Advantage is taken of the fact that K0(kr)K_0(kr) is a fundamental solution and J0(kr)J_0(kr) is the Riemann function of partial differential equations on the Euclidean plane

    The inner kernel theorem for a certain Segal algebra

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    The Segal algebra S0(G){\textbf{S}}_{0}(G) is well defined for arbitrary locally compact Abelian Hausdorff (LCA) groups GG. Despite the fact that it is a Banach space it is possible to derive a kernel theorem similar to the Schwartz kernel theorem, of course without making use of the Schwartz kernel theorem. First we characterize the bounded linear operators from S0(G1){\textbf{S}}_{0}(G_1) to S0â€Č(G2){\textbf{S}}_{0}'(G_2) by distributions in S0â€Č(G1×G2){\textbf{S}}_{0}'(G_1 \times G_2). We call this the "outer kernel theorem". The "inner kernel theorem" is concerned with the characterization of those linear operators which have kernels in the subspace S0(G1×G2){\textbf{S}}_{0}(G_1 \times G_2), the main subject of this manuscript. We provide a description of such operators as regularizing operators in our context, mapping S0â€Č(G1){\textbf{S}}_{0}'(G_1) into test functions in S0(G2){\textbf{S}}_{0}(G_2), in a w∗w^{*}-to norm continuous manner. The presentation provides a detailed functional analytic treatment of the situation and applies to the case of general LCA groups, without recurrence to the use of so-called Wilson bases, which have been used for the case of elementary LCA groups. The approach is then used in order to describe natural laws of composition which imitate the composition of linear mappings via matrix multiplications, now in a continuous setting. We use here that in a suitable (weak) form these operators approximate general operators. We also provide an explanation and mathematical justification used by engineers explaining in which sense pure frequencies "integrate" to a Dirac delta distribution

    Drawing graphs with vertices and edges in convex position

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    A graph has strong convex dimension 22, if it admits a straight-line drawing in the plane such that its vertices are in convex position and the midpoints of its edges are also in convex position. Halman, Onn, and Rothblum conjectured that graphs of strong convex dimension 22 are planar and therefore have at most 3n−63n-6 edges. We prove that all such graphs have at most 2n−32n-3 edges while on the other hand we present a class of non-planar graphs of strong convex dimension 22. We also give lower bounds on the maximum number of edges a graph of strong convex dimension 22 can have and discuss variants of this graph class. We apply our results to questions about large convexly independent sets in Minkowski sums of planar point sets, that have been of interest in recent years.Comment: 15 pages, 12 figures, improved expositio
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