Restricted Radon Transforms and Unions of Hyperplanes

Restricted Radon Transforms and Unions of Hyperplanes

RESTRICTED RADON TRANSFORMS AND UNIONS OF HYPERPLANES Daniel M. Oberlin Department of Mathematics, Florida State University October 2004 1 Introduction x (n 1) n If Σ − is the unit sphere in R , the Radon transform Rf of a suitable function f on Rn is defined by (n 1) Rf(σ; t) = Z f(p + tσ) dmn 1(p) σ Σ − ; t R; − σ? 2 2 where the integral is with respect to (n 1)-dimensional Lebesgue measure on the − hyperplane σ?. We also define, for 0 < δ < 1, 1 Rδf(σ; t) = δ− Z f(x + tσ) dmn(x): [σ B(0;1)]+B(0,δ) ?\ The paper [5] is concerned with the mapping properties of R from Lp(Rn) into mixed norm spaces defined by the norms q=r 1=q 1 r Z hZ g(σ; t) dti dσ : Σ(n 1) j j − −∞ (n 1) Here dσ denotes Lebesgue measure on Σ − . The purpose of this paper is mainly to study the possibility of analogous mixed norm estimates when dσ is replaced (n 1) by measures dµ(σ) supported on compact subsets S Σ − having dimension < n 1. We are usually interested in the case r =⊆ and will mostly settle for estimates− of restricted weak type in the indices p and1 q and those only for f supported in a ball. The following theorem, which we regard as an estimate for a restricted Radon transform, is typical of our results here: Theorem 1. Fix α (1; n 1). Suppose µ is a nonnegative and finite Borel (n 1) 2 − measure on Σ − satisfying the Frostman condition dµ(σ1)dµ(σ2) Z Z α < : (n 1) (n 1) σ1 σ2 1 Σ − Σ − j − j Typeset by -TEX AMS 1 2 DANIEL M. OBERLIN Then (n 1) 1/α 1=2 (1) λ µ σ Σ − : sup RχE(σ; t) > λ . E f 2 t R g j j 2 for λ > 0 and Borel E B(0; 1). That is, ⊆ α, 1=2 RχE Lµ 1(L ) . E : k k 1 j j Suppose that α (0; n 1). Say that a Borel set E Rn satisfies the (Besicov- 2 − ⊆ (n 1) itch) condition B(n 1; α) if there is a compact set S Σ − having Hausdorff dimension α such that− for each σ S there is a translate⊆ of an (n 1)-plane or- thogonal to σ which intersects E in2 a set of positive (n 1)-dimensional− Lebesgue measure. It is well-known that, given (0; α), such an− S supports a probability measure µ satisfying the hypothesis of Theorem2 1, but with α in place of α. In conjunction with Theorem 1, standard arguments imply that− such an E must have positive n-dimensional Lebesgue measure. That is, B(n 1; α) sets in Rn have positive Lebesgue measure if α > 1. As will be pointed out in− 2, the next theorem implies that, for α (0; 1) and in certain cases, B(n 1; α)x sets have Hausdorff dimension at least n2 1+α. (Here is a notational comment:− E will usually denote the Lebesgue measure− of E with the appropriate dimensionj beingj clear from the context.) Theorem 2. Suppose α (0; 1). Suppose µ is a nonnegative measure on a compact interval J R which satisfies2 the condition ⊆ e µ(I) I α . j j e for subintervals I J. Let µ be the image of µ under a one-to-one and bi-Lipschitz ⊆ (n 1) mapping of J into Σ − . If 0 < γ < β < α ande 1 1 + β γ 1 1 + γ 1 γ = − ; = ; η = − p 1 + 2β γ q 1 + 2β γ 1 + 2β γ − − − then there is the estimate q; 1=p η RδχE Lµ 1(L ) . E δ− k k 1 j j for Borel E B(0; 1) and δ (0; 1). ⊂ 2 Contrasting with Theorems 1 and 2, the next result provides a global estimate for a restricted Radon transform: Theorem 3. Suppose n 4. Let S be the (n 2)-sphere ≥ − n 1 − σ = (σ : : : ; σ ) Σ(n 1) : σ2 = σ2 1 n − X j n f 2 1 g and let µ be Lebesgue measure on S. Then there is an estimate (n 1)=n Rχ n 2 E E L − (L ) . − k k µ 1 j j RESTRICTED RADON TRANSFORMS AND UNIONS OF HYPERPLANES 3 for Borel E Rn. ⊆ This result is an analogue of (3) in [5] (which is a similar estimate but with µ (n 1) replaced by Lebesgue measure on Σ − and q = n). The proof of Theorem 3 parallels the proof in [5] but requires the L2 Fourier restriction estimates for the light cone in Rn in place of an easier L2 estimate used in [5]. The remainder of this paper is organized as follows: 2 contains the proofs of Theorems 2 and 3 and the statement and proof of a similarx result in the case when d is an integer strictly between 1 and n 1 and µ is Lebesgue measure on (n 1) − a suitable d-manifold in Σ − ; 3 contains the proof of Theorem 3; 4 contains some miscellaneous observations andx remarks: an analogue for Kahane'sx notion of Fourier dimension of Theorem 2 when n = 2 and examples bearing on the question of whether B(n 1; 1) sets in Rn must have positive measure or only full dimension (the answer depends− on the set S of directions). 2 Proofs of Theorems 1 and 2 x As Theorem 1 is a consequence of its analogue, uniform in δ (0; 1), for the 2 operators Rδ, we will restrict our attention to these operators. A standard method for obtaining restricted weak type estimates is to estimate E from below. We will do this with a particularly simple-minded strategy based onj j two observations and originally employed in [3] and [4]. The first observation is that N N n=1 En En Em En : Xn=1 X1 m<n N j [ j ≥ j j − ≤ ≤ j \ j (n 1) δ The second is the well-known fact that if σ Σ − and if, for t R, P denotes 2 2 σ a plate [σ? B(0; 1)] + B(0; δ) + tσ, then \ C(n)δ2 P δ P δ σ1 σ2 j \ j ≤ σ1 σ2 j − j (so long as σ1 and σ2 are not too far apart, an hypothesis we tacitly assume since it can be acheived by multiplying the measures µ appearing below by an appropriate partition of unity). Thus if, for n = 1;:::;N, we have plates P δ satisfying E σn δ j \ P C1λδ, it follows that σn j ≥ 2 1 (2) E C1Nλδ C(n)δ : j j ≥ − X σm σn 1 m<n N ≤ ≤ j − j Our strategy, then, will be to choose N and (n 1) σn σ Σ − : sup RδχE(σ; t) > λ 2 f 2 t R g 2 so that (2) gives, for example, 2 (n 1) 2/α E & λ µ σ Σ − : sup RδχE(σ; t) > λ ; j j f 2 t R g 2 which is the analogue of (1) for the operator Rδ. For Theorem 1 the following lemma will facilitate this choice: 4 DANIEL M. OBERLIN Lemma 1. Let µ be as in Theorem 1. There is C = C(µ) such that given n N (n 1) 2 and a Borel S Σ − with µ(S) > 0, one can choose σn S, 1 n N, such that ⊆ 2 ≤ ≤ 1 CN 2 : 2/α X σm σn ≤ µ(S) 1 m<n N ≤ ≤ j − j Proof of Lemma 1: Suppose σ1; : : : ; σN are chosen independently and at random from the probability space (S; µ ). Then, for 1 m < n N, µ(S) ≤ ≤ 1 1 1 E = 2 Z Z dµ(σm) dµ(σn) σm σn µ(S) σm σn ≤ j − j S S j − j 1 1 1/α 1 1/α C 1 dµ(σ )dµ(σ ) − dµ(σ )dµ(σ ) ; 2 Z Z m n Z Z α m n 2/α µ(S) σm σn ≤ µ(S) S S S S j − j by the hypothesis on µ. Thus 1 CN 2 E 2/α X1 m<n N σm σn ≤ µ(S) ≤ ≤ j − j and the lemma follows. Proof of Theorem 1: Let S be the set (n 1) σ Σ − : sup RδχE(σ; t) > λ f 2 t R g 2 δ so that if σ S then there is t R such that if Pσ = [σ? B(0; 1)] + B(0; δ) + tσ 2δ 2 \ then E P C1λδ. The conjunction of Lemma 1 and (2) yields j \ σ j ≥ 2 2 2α (3) E C1Nλδ C2δ N µ(S)− : j j ≥ − : 2/α We consider two cases (noting that N = N0 = λC1µ(S) =C2δ makes the RHS of (3) equal to 0): Case I: Assume N0 > 10. In this case choose N N such that 2 λC µ(S)2/α λC µ(S)2/α 1 N 1 : 2C2δ ≥ ≥ 3C2δ Then it follows from (3) that 2/α 2 2 4/α λC1µ(S) 2 λ C1 µ(S) 2/α 2 2/α E C1 λδ C2δ 2 2 µ(S)− = κλ µ(S) j j ≥ 3C2δ − 4C2 δ 2 1/α 1=2 for κ = C =(12C2). This gives λµ(S) E as desired. 1 . j j Case II: Assume N0 10. In this case (unless S≤is empty) we estimate 2 2 2/α λ C1 µ(S) E C1λδ j j ≥ ≥ 10C2 RESTRICTED RADON TRANSFORMS AND UNIONS OF HYPERPLANES 5 which again yields λ µ(S)1/α E 1=2 and so completes the proof of Theorem 1.

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