2015
DOI: 10.1515/crelle-2015-0023
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Kinematic formulas for tensor valuations

Abstract: We prove new kinematic formulas for tensor valuations and simplify previously known Crofton formulas by using the recently developed algebraic theory of translation invariant valuations. The heart of the paper is the computation of the Alesker-Fourier transform on the large class of spherical valuations, which is achieved by differential-geometric and representation theoretical tools. We also describe in explicit form the product and convolution of tensor valuations.

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Cited by 46 publications
(71 citation statements)
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References 51 publications
(110 reference statements)
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“…The tensor Cm is equal to a linear combination of the Minkowski tensor W10,2 (which is defined below, see Tables I and II) and the unit tensor multiplied by the surface area (or the perimeter for d = 2). The coefficients are explicitly given by so‐called Crofton formulas for Minkowski tensors . For local versions of these Crofton formulas, see Ref.…”
Section: Mean Intercept Length Of Anisotropic Boolean Modelsmentioning
confidence: 99%
See 1 more Smart Citation
“…The tensor Cm is equal to a linear combination of the Minkowski tensor W10,2 (which is defined below, see Tables I and II) and the unit tensor multiplied by the surface area (or the perimeter for d = 2). The coefficients are explicitly given by so‐called Crofton formulas for Minkowski tensors . For local versions of these Crofton formulas, see Ref.…”
Section: Mean Intercept Length Of Anisotropic Boolean Modelsmentioning
confidence: 99%
“…The coefficients are explicitly given by so-called Crofton formulas for Minkowski tensors. 41,42 For local versions of these Crofton formulas, see Ref. [43].…”
Section: F Generalized Anisotropy Measuresmentioning
confidence: 99%
“…Tensor valuations on convex bodies have attracted increasing attention in recent years (see, e.g., [7,23,26]). They were introduced by McMullen in [37] and Alesker subsequently obtained a complete classification of continuous and isometry equivariant tensor valuations on convex bodies (based on [3] but completed in [4]).…”
Section: Introduction and Statement Of Resultsmentioning
confidence: 99%
“…Formula (20) follows from (19) if sin t = 0, and hence by the continuity of Z m if sin t = 0. Now Z m is smooth because it is invariant under SU(m) (see Proposition 3.6), and ϕ t ∈ GL(2m, R), t ∈ (− π 2 , π 2 ), is a C ∞ family of 2m × 2m matrices, thus Z m (ϕ t K) is a C ∞ function of t. Since Z m (ϕ t K) is differentiable at t = 0, but the right-hand-side of (20) is differentiable only if it vanishes, we conclude Kl Zm (L) = 0 by (20).…”
Section: Case J = Mmentioning
confidence: 99%