Results on fractal measure of some sets

The fractal dimensions are very important characteristics of fractal sets. A problem which arises in the study of fractal sets is the determination of their dimensions. The Hausdorf dimension is dfficult to be determined, even if the box dimensions can be computed. In this article we present some re...

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Zitieren:Results on fractal measure of some sets / A. Barbulescu // Theory of Stochastic Processes. — 2007. — Т. 13 (29), № 1-2. — С. 13-22. — Бібліогр.: 13 назв.— англ.

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spelling irk-123456789-44732009-11-20T12:00:55Z Results on fractal measure of some sets Barbulescu, A. The fractal dimensions are very important characteristics of fractal sets. A problem which arises in the study of fractal sets is the determination of their dimensions. The Hausdorf dimension is dfficult to be determined, even if the box dimensions can be computed. In this article we present some relations between these types of measures and we estimate them for some sets. 2007 Article Results on fractal measure of some sets / A. Barbulescu // Theory of Stochastic Processes. — 2007. — Т. 13 (29), № 1-2. — С. 13-22. — Бібліогр.: 13 назв.— англ. 0321-3900 http://dspace.nbuv.gov.ua/handle/123456789/4473 en Інститут математики НАН України
institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
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description The fractal dimensions are very important characteristics of fractal sets. A problem which arises in the study of fractal sets is the determination of their dimensions. The Hausdorf dimension is dfficult to be determined, even if the box dimensions can be computed. In this article we present some relations between these types of measures and we estimate them for some sets.
format Article
author Barbulescu, A.
spellingShingle Barbulescu, A.
Results on fractal measure of some sets
author_facet Barbulescu, A.
author_sort Barbulescu, A.
title Results on fractal measure of some sets
title_short Results on fractal measure of some sets
title_full Results on fractal measure of some sets
title_fullStr Results on fractal measure of some sets
title_full_unstemmed Results on fractal measure of some sets
title_sort results on fractal measure of some sets
publisher Інститут математики НАН України
publishDate 2007
url http://dspace.nbuv.gov.ua/handle/123456789/4473
citation_txt Results on fractal measure of some sets / A. Barbulescu // Theory of Stochastic Processes. — 2007. — Т. 13 (29), № 1-2. — С. 13-22. — Бібліогр.: 13 назв.— англ.
work_keys_str_mv AT barbulescua resultsonfractalmeasureofsomesets
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fulltext Theory of Stochastic Processes Vol.13 (29), no.1-2, 2007, pp.13-22 ALINA BARBULESCU RESULTS ON FRACTAL MEASURE OF SOME SETS The fractal dimensions are very important characteristics of fractal sets. A problem which arises in the study of fractal sets is the deter- mination of their dimensions. The Hausdorff dimension is difficult to be determined, even if the box dimensions can be computed. In this article we present some relations between these types of measures and we estimate them for some sets. 1. Introduction The dimensions calculus is fundamental in the fractals study. The Haus- dorff measures, the box and packing dimensions are widely used and in many papers the relations between them are given ([5] - [7], [11]). In [1] - [4] we gave some boundedness conditions for a class of fractal sets, in Rn. This type of conditions is important in order to prove theorems concerning the module and the capacities and the relations between them ([10]) or to determine the dimensions of fractal sets ([8], [9], [12], [13]). In what follows we shall work with the following basic notions. Definition 1. Let Rn be the Euclidean n-dimensional metric space, E a subset of Rn and r0 > 0. A continuous function h(r), defined on [0, r0) , nondecreasing and such that lim r→0 h(r) = 0 is called a measure function. If 0 < β < ∞ and h is a measure function, then, the Hausdorff h-measure of E is defined by : Hh(E) = lim β→0 inf {∑ i h(|Ui|) : E ⊆ ⋃ i Ui : 0 < |Ui| < β } . where |Ui| is the diameter of Ui. 2000 Mathematics Subject Classifications 28A78 Key words and phrases. Hausdorff h-measure, box dimension, boundedness 13 14 ALINA BARBULESCU Remark. There are definitions where the cover of the set E is made with balls. The relation between these ”spherical” Hausdorff h - measure, de- noted by H ′ h and Hh is: Hh(E) ≤ H ′ h(E). (1) Definition 2. Let ϕ1, ϕ2 > 0 be functions defined in D ⊂ Rn. We say that ϕ1 and ϕ2 are similar and we denote by: ϕ1 ∼ ϕ2, if there exists Q > 0, satisfying: 1 Q ϕ1(x) ≤ ϕ2(x) ≤ Qϕ1(x), ∀x ∈ D. Definition 3. Let δ > 0 and f : D ⊂ Rn → R. f is said to be a δ - class Lipschitz function if there exists M > 0 such that: |f(x + α) − f(x)| ≤ M‖α‖δ, ∀x ∈ D, ∀α ∈ Rn withx + α ∈ D, where for α ∈ Rn, α = (α1, ..., αn), ‖α‖ = ∑n i=1 α2 i . f is said to be a Lipschitz function if δ = 1. Definition 4. A set E ⊂ Rn is called k - rectifiable if there are a Lipschitz function f : Rk → Rn and a bounded subset F of Rk, such that f (F ) =E. If f : [0, 1] → R, we denote by Rf [t1, t2] the oscillation of f on [t1, t2] ⊂ [0, 1] and by Γ (f) the graph of the function f . 2. Results In ([1] − [3]), the following functions were studied: g(x) = ⎧⎪⎪⎨ ⎪⎪⎩ 2x , 0 ≤ x < 1 2 −2 (x − 1) , 1 2 ≤ x < 3 2 2(x − 2) , 3 2 ≤ x < 2 (2) f(x) = ∞∑ i=1 λs−2 i g(λix), (∀)x ∈ [0, 1] , (3) where g is given in (2), s > 0 and {λi}i∈N∗ is a sequence such that (∃) ε > 1 : λi+1 ≥ ελi > 0, (∀) i ∈ N∗. (4) Theorem 1. ([2]) If h is a measure function, h(t)˜tp, p ≥ 2, f : [0, 1] → R is a δ- class Lipschitz function, δ ≥ 0, then Hh(Γ(f)) < +∞. The result RESULTS ON FRACTAL MEASURE OF SOME SETS 15 remains true if p ≥ 1 and δ > 1. Theorem 2. If h is a measure function, h(t)˜tp, p ≥ 2, f is the function defined in (3), with s ∈ [0 , 2) and {λi}i∈N∗ ∈ R+ is a sequence that satis- fies (4), then Hh(Γ(f)) < +∞. Proof. For s ∈ [1 , 2), the proof is analogous to that of theorem 2 [1]. It remains to prove the result for s ∈ [0 , 1) . We consider 0 < α < 1, small enough and k ∈ N∗ such that: λ−1 k+1 ≤ α < λ−1 k . (5) Then: |f(x + α) − f(x)| = ∣∣∣∣∣ ∞∑ i=1 λs−2 i {g(λi(x + α)) − g(λix)} ∣∣∣∣∣ ≤ ≤ k∑ i=1 λs−2 i |g(λi(x + α)) − g(λix)| + ∞∑ i=k+1 λs−2 i |g(λi(x + α)) − g(λix)| . From the definition of g it results: |g(λi(x + α)) − g(λix)| ≤ 2. Thus: |f(x + α) − f(x)| ≤ k∑ i=1 λs−2 i |g(λi(x + α)) − g(λix)| + 2 ∞∑ i=k+1 λs−2 i ⇒ |f(x + α) − f(x)| ≤ 2α k∑ i=1 λs−1 i + 2 ∞∑ i=k+1 λs−2 i . (6) Using (4) we have: εi−1λ1 < λi , s < 1 ⇒ λs−1 i < λs−1 1 ( εi−1 )s−1 ⇒ k∑ i=1 λs−1 i < λs−1 1 k∑ i=1 ( εs−1 )i−1 = λs−1 1 1 − (1 ε )k(1−s) 1 − (1 ε )1−s ⇒ k∑ i=1 λs−1 i < λs−1 1 · 1 1 − (1 ε )1−s . (7) The relations (6) and (7) give: |f(x + α) − f(x)| ≤ α 2λs−1 1 1 − (1 ε )1−s + 2 ∞∑ i=k+1 λs−2 i . (8) 16 ALINA BARBULESCU ∞∑ i=k+1 λs−2 i ≤ ∞∑ j=0 ( εjλk+1 )s−2 = λs−2 k+1 ∞∑ j=0 ( εj )s−2 = λs−2 k+1 ∞∑ j=0 ( εs−2 )j Since s − 2 < 0, ε > 1, the series ∞∑ j=0 (εs−2) j is convergent and ∞∑ i=k+1 λs−2 i < λs−2 k+1 · 1 1 − (1 ε )2−s (9) From (8) and (9), it results: |f(x + α) − f(x)| ≤ α 2λs−2 1 1 − (1 ε )1−s + 2λs−2 k+1 1 − (1 ε )2−s (10) The relation (5) implies: λs−2 k+1 ≤ α2−s < α because α ∈ [0, 1) . Thus: |f(x + α) − f(x)| ≤ α ( 2λs−1 1 1 − (1 ε )1−s + 2 1 − (1 ε )2−s ) = αM ⇔ |f(x + α) − f(x)| < αM, (11) where M = 2λs−1 1 1−( 1 ε) 1−s + 2 1−( 1 ε) 2−s . From (11) it results that f is a Lipschitz function. Since the hypothesis of the theorem 1 is satisfied, then Hh(Γ(f)) < +∞. Theorem 3. Let h be a measure function, such that h(t)˜P (t)eT (t), t ≥ 0, (12) where P and T are polynomials: P (t) = a1t + a2t 2 + ... + apt p, p ≥ 1, T (t) = b0 + b1t + ... + amtm, with the property P ′ (t) + P (t) · T (t) > 0, t ≥ 0. (13) If f : [0, 1] → R is a δ - class Lipschitz function, δ ≥ 1, then Hh(Γ(f)) < +∞. The result remains true if p ≥ 2, a1 = 0 and δ ∈ [0, 1] . Proof. The condition (13) means that P (t)eT (t), t ≥ 0 is itself a measure function. The first part of the proof follows that of [5] . RESULTS ON FRACTAL MEASURE OF SOME SETS 17 We suppose that the Lipschitz constant is M = 1. To any x corresponds an interval (x− k, x + k) such that, for any x + α of this interval: |f(x + α) − f(x)| ≤ |α|δ . Since [0, 1] is a compact set, there exists a finite set of overlapping in- tervals covering (0, 1): (0, k0), (x1 − k1, x1 + k1), ..., (xn−1 − kn−1, xn−1 + kn−1), (1 − kn, 1). If ci are arbitrary points, satisfying: c1 ∈ (0, x1), ci ∈ (xi−1, xi), i = 2, ..., n − 1, cn ∈ (xn−1, 1) ci ∈ (xi−1 − ki−1, xi−1 + ki−1) ⋂ (xi − ki, xi + ki), i = 2, ..., n − 1. we have: 0 < c1 < x1 < c2 < x2 < ... < xn−1 < cn < 1· The oscillation of f(x) in the interval (ci−1, ci) is less than 2 (ci − ci−1) δ and thus the part of the curve corresponding to the interval (ci−1, ci) can be enclosed in a rectangle of height 2 (ci − ci−1) δ and of base ci − ci−1, and consequently in [ 2 (ci − ci−1) δ−1 ] + 1 squares of side ci − ci−1 or in the number of circles of radius ci−ci−1√ 2 circumscribed about each of these squares. The integer part of x was denoted by [x]. Given an arbitrary r ∈ (0, 1 2 ) it can always be assumed that: ci−ci−1 < r, i = 2, 3, ..., n. Denote by Cr the set of all the above circles and consider ∑ Cr h(2r) = ∑ Cr { h(2r) eT (2r) · P (2r) · eT (2r) · P (2r) } . From (12) it results that: (∃)Q > 0 : h(2r) eT (2r) · P (2r) ≤ Q. Then, ∑ Cr h(2r) ≤ Q ∑ Cr { eT (2r) · P (2r) }⇔ ∑ Cr h(2r) ≤ Q ∑ Cr P (2r) · e m k=0 bk·(2r)k . r ∈ ( 0, 1 2 ) ⇒ ∑ Cr h(2r) ≤ Q · e m k=0|bk| · ∑ Cr P (2r)· We have to estimate ∑ Cr P (2r). 18 ALINA BARBULESCU The sum of the terms corresponding to the interval (ci−1, ci), i = 2, ..., n is: Si = {[ 2 (ci − ci−1) δ−1 ] + 1 } · p∑ k=1 ak { (ci − ci−1) √ 2 }k , where [x] is the integer part of x. Si ≤ { 2 (ci − ci−1) δ−1 + 1 } · p∑ k=1 { ak · (ci − ci−1) k · 2k/2 } ⇒ Si ≤ 2 p 2 · max k∈1, p |ak| · p∑ k=1 { 2 (ci − ci−1) k+δ−1 + (ci − ci−1) k } ci − ci−1 < 1, k + δ − 1 ≥ 1 ⇒ (ci − ci−1) k+δ−1 ≤ ci − ci−1 ⇒ Si ≤ 3 · 2 p 2 · p · max k∈1, p |ak| (ci − ci−1) ⇒ ∑ Cr P (2r) ≤ 3 · 2 p 2 · p · max k∈1, p |ak| n∑ i=2 (ci − ci−1) ≤ 3 · 2 p 2 · p · max k∈1, p |ak| ⇒ ∑ Cr h(2r) ≤ 3 · 2 p 2 · p · Q · max k∈1, p |ak| · e m k=0|bk|. Then H ′ h(Γ(f)) < +∞ ⇒ H ′ h(Γ(f)) < +∞. If M �= 1, then∑ Cr h(2r) ≤ 3 · 2 p 2 · p · Q · M · max k∈1, p |ak| · e m k=0|bk | ⇒ Hh(Γ(f)) < +∞. If p ≥ 2 and δ > 0, then k ≥ 2,(ci − ci−1) k+δ−1 < ci − ci−1 and the proof is the same as above. Theorem 4. If Γ(f) is the graph of the function defined in (3), s ∈ [0, 2), {λi}i∈N∗ ∈ R+ is a sequence of numbers, that satisfies (4) and h is a measure function satisfying (12), then Hh(Γ(f)) < +∞. Proof. The proof is analogous to that of the Theorem 3. The following lemma will be used: Lemma 1. ([6]) Let f ∈ C [0, 1] , 0 < β < 1 and m be the least integer greater than or equal to 1/β. If Nβ(Γ(f)) is the number of the squares of the β− mesh that intersects Γ (f) , then β−1 m−1∑ j=0 Rf [jβ, (j + 1)β] ≤ Nβ(Γ(f)) ≤ 2m + β−1 m−1∑ j=0 Rf [jβ, (j + 1)β] . RESULTS ON FRACTAL MEASURE OF SOME SETS 19 Let us consider δ > 0 and a δ - class Lipschitz function, f : [0, 1] → R. Then: |f(x) − f(y)| ≤ M |x − y|δ, (∀)x, y ∈ [0, 1]. Rf [jβ, (j + 1)β] = sup jβ≤t, u≤(j+1)β |f (t) − f (u)| ⇒ Rf [jβ, (j + 1)β] ≤ M sup jβ≤t, u≤(j+1)β |t − u|δ ⇒ Rf [jβ, (j + 1)β] ≤ Mβδ. Let N ′ β(Γ(f)) be the number of β - mesh squares that cover the set Γ(f). Denoting by [x], the integer part of x ∈ R and using lemma 1, it can be deduced that: N ′ β(Γ(f)) ≤ 2 [ 1 β ] + β−1 [ 1 β ] Mβδ ⇒ N ′ β(Γ(f)) < Mβδ−2 + 2 β . (14) But, Nβ √ n(Γ(f)) ≤ N ′ β(Γ(f)) ≤ 2nNβ(Γ(f)), (15) where Nβ(Γ(f)) is the smallest number of discs of diameters at most β that cover Γ(f). The relations (14) and (15) give for n = 2: Nβ(Γ(f)) ≤ N ′ β√ 2 (Γ(f)) < M ( β√ 2 )δ−2 + 2 √ 2 β ⇒ Nβ(Γ(f)) ≤ N ′ β√ 2 (Γ(f)) < 3 β + M ′βδ−2, (16) with M ′ = M√ 2 δ−2 . Theorem 5. If f : [0, 1] → R is a δ-class Lipschitz function, δ > 0 and h is a measure function such that h(t) ∼ tp, p > 2, then Hh(Γ(f)) = 0. The assertion remains true if p ≥ 1 and δ > 1. Proof. By hypotheses, Γ(f) is a compact set. Therefore, if β > 0, for every cover of Γ(f) with open discs Ui, i ∈ N∗, with diameters di ≤ β, there is a finite number of discs, nβ, that covers Γ(f). H ′ h(Γ(f)) = lim β→0 inf {∑ i h(|Ui|) : E ⊆ ⋃ i Ui : 0 < |Ui| ≤ β } = 20 ALINA BARBULESCU = lim β→0 inf { nβ∑ i=1 h(|Ui|) } ≤ lim β→0 inf {h(β)nβ} , since h is nondecreasing. Then H ′ h(Γ(f)) ≤ lim β→0 {h(β)Nβ(Γ(f))} , where Nβ(Γ(f)) is the smallest number of open discs of diameters at most β that cover Γ(f). Denoting by N ′ β(Γ(f)) the number of β - mesh squares that cover Γ(f) and using the relations (1) and (16), the previous inequality becomes: Hh(Γ(f)) ≤ H ′ h(Γ(f)) ≤ lim β→0 { h(β)N ′ β√ 2 (Γ(f)) } ⇒ Hh(Γ(f)) ≤ lim β→0 { h(β)(3β−1 + M ′βδ−2) }⇒ Hh(Γ(f)) ≤ lim β→0 { h(β) βp (3βp−1 + M ′βp+δ−2) } . Since h(t) ∼ tp, p > 2, there is Q > 0 such that: 1 Q tp ≤ h(t) ≤ Qtp, and then Hh(Γ(f)) ≤ Qlim β→0 (3βp−1 + M ′βp+δ−2) = 0, because p − 1 > 0 and p + δ − 2 > 0. So, Hh(Γ(f)) = 0. If p ≥ 1 and δ > 1 the proof is the same because p + δ − 2 > 0. Remark. Theorem 5 gives a better result as the theorem 6 [2], where it was proved in the same hypotheses, that H ′ h(Γ(f)) < ∞. Lemma 2. ([4]) If E ⊂ Rm, F ⊂ Rn, f : E → F is a surjective Lipschitz function, with the Lipschitz constant M and h is a measure function, then: Hh(F ) ≤ Hh(M · E). Theorem 6. If E ⊂ Rn is a k-rectifiable set and h is a measure function such that h(t) ∼ tp, p > 2, then Hh(E) = 0. Proof. If E ⊂ Rn is k - rectifiable, there exists a bounded set G ⊂ Rk and f : Rk → Rn such that: ‖f(x) − f(y)‖ < M‖x − y‖, (∀)x, y ∈ Rk RESULTS ON FRACTAL MEASURE OF SOME SETS 21 and f(G) = E. The restriction of f at G is a surjection and, by Lemma 2, Hh(f(G)) ≤ Hh(M · G) ⇔ Hh(E) ≤ Hh(M · G). M ·G is bounded, so there is a disc B(z0, r), (r > 0) such that M ·G ⊂ B(z0, r). Therefore, Hh(E) ≤ H ′ h(E) ≤ H ′ h(B(z0, r)) = = lim β→0 inf {∑ i h(|Ui|) : B(z0, r) ⊆ ⋃ i Ui : 0 < |Ui| ≤ β } = = lim β→0 inf {nβ · h(|Ui|)} , where nβ is the number of the open discs Ui with the diameters |Ui| ≤ β, that covers B(z0, r). nβ ≥ π · r2 π·|Ui|2 4 = 4 · r2 |Ui|2 ⇒ Hh(E) ≤ H ′ h(B(z0, r)) ≤ lim β→0 inf {nβ · h(β)} = = lim β→0 h(β) inf nβ = lim β→0 h(β) · 4r2 β2 = 4r2 lim β→0 h(β) β2 = = 4r2 lim β→0 { h(β) βp · βp−2 } ≤ 4Qr2 lim β→0 βp−2 = 0, where it was used that h(t) ∼ tp, p > 2. So, Hh(E) = 0. Remark. If in Theorem 6, p = 2, it results that Hh(E) ≤ 4Qr2, so the Hausdorff h-measure of the k - rectifiable set E is finite. Bibliography 1. Bărbulescu, A., La finitude d’une h-mesure Hausdorff d’un ensemble de points dans le plan, Ann. Univ. Valahia Targoviste, 1995/1996, fasc.II, 93–99. 2. Bărbulescu, A., On the h-measure of a set, Revue Roumaine de Mathémati- que pures and appliquées, tome XLVII, 5–6, (2002), 547–552. 3. Bărbulescu, A., New results about the h-measure of a set, Analysis and Optimization of Differential Systems, Kluwer Academic Publishers, (2003), 43–48. 4. Bărbulescu, A., About some properties of the Hausdorff measure, Proceed- ings of the 10-th Symposium of Mathematics and its applications, Novem- ber, 6–9, 2003, Timisoara, Romania, 17–22 22 ALINA BARBULESCU 5. Besicovitch, A. S., Ursell H. D., Sets of fractional dimension (V): On di- mensional numbers of some continuous curves, London Math. Soc. J., 12, (1937), 118–125 6. Falconer K. J., The geometry of fractal sets, Cambridge Tracts in Mathe- matics, Cambridge University (1985) 7. Falconer K. J., Fractal geometry: Mathematical foundations and applica- tions, J.Wiley & Sons Ltd., (1990) 8. Hutchinson J.E., Fractals and Self Similarity, Indiana University Math. Journal, vol. 30, no. 5 (1981), 713–747 9. Moran, P. A. P. Additive functions of intervals and Hausdorff measure, Proceedings of Cambridge Phil. Soc., vol. 42, (1946), 15–23 10. Taylor S. J., On the connection between Hausdorff measures and gen- eralized capacity, Proceedings of Cambridge Phil. Soc., vol. 57, (1961), 524–531 11. Xie T.F., Zhou S.P., On a class of fractal functions with graph Box dimension 2, Chaos, Solitons and Fractals, 22 (2004), 135–139 12. Yao K., Su W.Y., Zhou S.P., On the connection between the order of fractional calculus and the dimensions of a fractal function, Chaos, Solitons and Fractals, 23 (2005), 621–629 13. Zhou S.P., He G.L., Xie T.F., On a class of fractals; the constructive structure, Chaos, Solitons and Fractals, 19 (2004), 1099–1104 Department of Mathematics, Ovidius University of Constanta, 900527 Constanta, Romania. E-mail address: abarbulescu@univ-ovidius.ro