1997
DOI: 10.1090/s0002-9939-97-03570-3
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Radon transform on spaces of constant curvature

Abstract: Abstract. A correspondence among the totally geodesic Radon transformsas well as among their duals-on the constant curvature spaces is established, and is used here to obtain various range characterizations.

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Cited by 16 publications
(10 citation statements)
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“…The case j = 0 corresponds to the totally geodesic transform R k : h → ζ h that takes functions on H n to functions on G H (n, k); cf. [1,2,20,21,26,35,50]. The corresponding dual transform is defined by…”
Section: Radon Transforms Of Zonal Functionsmentioning
confidence: 99%
See 1 more Smart Citation
“…The case j = 0 corresponds to the totally geodesic transform R k : h → ζ h that takes functions on H n to functions on G H (n, k); cf. [1,2,20,21,26,35,50]. The corresponding dual transform is defined by…”
Section: Radon Transforms Of Zonal Functionsmentioning
confidence: 99%
“…The corresponding formulas for totally geodesic submanifolds and the relevant Radon transforms require substantial technical work related to computation of Jacobians; cf. [2,26], [39, pp. 412-416].…”
Section: Introductionmentioning
confidence: 99%
“…Theorems of the previous section can be converted into the similar statements for the Funk type transforms on the sphere and Grassmann manifolds by making use of the stereographic projection. A remarkable interrelation between diverse integral operators on R n and S n is known for many years and the corresponding transition formulas can be found in numerous publications; see, e.g., Mikhlin [45,, Berenstein, Casadio Tarabusi and Kurusa [4], Drury [23], Rubin [56, Section 5.2], to mention a few. Below we recall the reasoning from our paper [54] which has proved to be especially helpful in the general context of Grassmannians.…”
Section: More Generally Assumingmentioning
confidence: 99%
“…Using the projective equivalence of the operator (7.2) and the hyperplane Radon transform R, as in [22,Lemma 8.3] (see also [13,3]), we obtain the following kernel description, which is implied by Theorem 3.7. We write x ∈ H n in the hyperbolic polar coordinates as x = θ sinhr + e n+1 coshr, θ ∈ S n−1 , r > 0, and consider the Fourier-Laplace coefficients f m,µ (r) =…”
Section: The Totally Geodesic Radon Transform On the Hyperbolic Spacementioning
confidence: 99%