2016
DOI: 10.1214/15-aap1097
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High-frequency asymptotics for Lipschitz–Killing curvatures of excursion sets on the sphere

Abstract: In this paper, we shall be concerned with geometric functionals and excursion probabilities for some nonlinear transforms evaluated on Fourier components of spherical random fields. In particular, we consider both random spherical harmonics and their smoothed averages, which can be viewed as random wavelet coefficients in the continuous case. For such fields, we consider smoothed polynomial transforms; we focus on the geometry of their excursion sets, and we study their asymptotic behaviour, in the high-freque… Show more

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Cited by 24 publications
(29 citation statements)
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References 62 publications
(113 reference statements)
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“…As an application of the previous result, let us consider the Fourier components false{f(·)false}=1,2, normalized to have variance one; the GKF yields immediately (compare Marinucci and Vadlamani (), Corollary 5, see also Cheng and Xiao ()).Efalse[L0(Aufalse(f(.);S2false))false]=21-Φ(u)+λ2ue-u2/2(2π)34π;Efalse[L1(Aufalse(f(.);S2false))false]=π212λ1/2e-u2false/22π4π=π2λ1/2e-u2/2;andEfalse[L2(Aufalse(f(.);S2false))false]=4π×1-Φ(u).…”
Section: Characterization Of Excursion Sets For Random Spherical Harmmentioning
confidence: 84%
“…As an application of the previous result, let us consider the Fourier components false{f(·)false}=1,2, normalized to have variance one; the GKF yields immediately (compare Marinucci and Vadlamani (), Corollary 5, see also Cheng and Xiao ()).Efalse[L0(Aufalse(f(.);S2false))false]=21-Φ(u)+λ2ue-u2/2(2π)34π;Efalse[L1(Aufalse(f(.);S2false))false]=π212λ1/2e-u2false/22π4π=π2λ1/2e-u2/2;andEfalse[L2(Aufalse(f(.);S2false))false]=4π×1-Φ(u).…”
Section: Characterization Of Excursion Sets For Random Spherical Harmmentioning
confidence: 84%
“…see [16]. For fixed j, as in (2) it follows from results in [1] that there exist α > 1 and µ + > 0 such that, for all u > µ + P sup…”
Section: Introductionmentioning
confidence: 99%
“…Spherical random fields have recently drawn a lot of applied interest, especially in an astrophysical environment (see [6], [14]); closed form expressions for the density of their maxima and for excursion probabilities have been given in ( [10], [9], [16]). In particular, the latter references exploit the Gaussian Kinematic Fundamental formula by Adler and Taylor (see [1]) to approximate excursion probabilities by means of the expected value of the Euler-Poincarè characteristic for excursion sets.…”
Section: Introductionmentioning
confidence: 99%
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