<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">JAMP</journal-id><journal-title-group><journal-title>Journal of Applied Mathematics and Physics</journal-title></journal-title-group><issn pub-type="epub">2327-4352</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jamp.2020.81009</article-id><article-id pub-id-type="publisher-id">JAMP-97688</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Dimension of the Non-Differentiability Subset of the Cantor Function
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Muquan</surname><given-names>Yan</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Department of Mathematics, South China University of Technology, Guangzhou, China</addr-line></aff><pub-date pub-type="epub"><day>26</day><month>12</month><year>2019</year></pub-date><volume>08</volume><issue>01</issue><fpage>107</fpage><lpage>114</lpage><history><date date-type="received"><day>30,</day>	<month>October</month>	<year>2019</year></date><date date-type="rev-recd"><day>5,</day>	<month>January</month>	<year>2020</year>	</date><date date-type="accepted"><day>8,</day>	<month>January</month>	<year>2020</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  The main purpose of this note is to estimate the size of the set 
  T<sub>μλ</sub> of points, at which the Cantor function is not differentiable and we find that the Hausdorff dimension of 
  T<sub>μλ</sub> is [log2/log3]
  <sup>2</sup>. Moreover, the Packing dimension of 
  T<sub>μλ</sub> is log2/log3. The log2 = log
  <sub>e</sub>2 is that if 
  a
  <sup>x</sup> = 
  N (
  a &gt;0, and 
  a≠1), then the number 
  x is called the logarithm of 
  N with a base, recorded as 
  x = log
  <sub>a</sub>
  N, read as the logarithm of 
  N with a base, where a is called logarithm Base number, 
  N is called true number.
 
</p></abstract><kwd-group><kwd>Hausdor Dimension</kwd><kwd> Packing Dimension</kwd><kwd> Cantor Ternary Function</kwd><kwd> Cantor Ternary Set</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Let T be the Cantor middle thirds set (Start with the closed interval [ 0,1 ] . Remove the open interval ( 1 3 , 2 3 ) to obtain [ 0, 1 3 ] ∪ [ 2 3 ,1 ] , i.e. two disjoint</p><p>closed segments. Remove the middle thirds of those two segments, and you end up with four disjoint segments. After infinitely many steps, the result is called the Cantor set.) and θ be the Cantor ternary function (The function can be defined in the following way, given x ∈ [ 0,1 ] consider its ternary expansion a i , i.e. a choice of coefficients a i ∈ { 0,1,2 } such that</p><p>x = ∑ i = 1 ∞ a i 3 i . (1.1)</p><p>Define n ( x ) to be ∞ if none of the coefficients a i takes the value 1 and the smallest integer n such that a n = 1 otherwise.</p><p>Then</p><p>f ( x ) = ∑ i = 1 n ( x ) − 1 a i 2 i + 1 + 1 2 n ( x ) . (1.2)</p><p>Let N * be the set of non-differentiable points of Cantor function θ .</p><p>Denote</p><p>θ − = lim inf r → 0 − θ ( t + r ) − θ ( t ) r . (1.3)</p><p>and</p><p>θ + = lim inf r → 0 + θ ( t + r ) − θ ( t ) r . (1.4)</p><p>See [<xref ref-type="bibr" rid="scirp.97688-ref1">1</xref>], we have</p><p>lim inf r → 0 θ ( t + r ) − θ ( t ) r = ∞ . (1.5)</p><p>So,</p><p>N * = { t ∈ T : θ − ( t ) &lt; ∞     or     θ + ( t ) &lt; ∞ } .</p><p>Let t = . t 1 t 2 ⋯ be the ternary expansion of a point in T, which is not an endpoint of a complementary interval. Let z ( n ) denote the position of the nth zero in this ternary expansion, and t ( n ) denote the position of the nth two in the expansion of t.</p><p>For each μ ≥ 0 and λ ≥ 0 , define</p><p>T μ λ = { t ∈ T : θ − ( t ) = μ   and   θ + ( t ) = λ } .</p><p>Firstly, several authors [<xref ref-type="bibr" rid="scirp.97688-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.97688-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.97688-ref4">4</xref>] have proved that the Hausdorff dimension of the set N * is ( log 2 / log 3 ) 2 and the packing dimension of N * is log 2 / log 3 .</p><p>Let the Cantor T in R be defined by T = ∪ j = 1 r h j ( T ) with a disjoint union, where</p><p>the h j are similitude mappings with ratios 0 &lt; a j &lt; 1 . Let μ be the self-similar Borel probability measure on T corresponding to the probability vector ( p 0 , p 1 , ⋯ , p r ) . Let S be the set of points at which the probability distribution function F ( x ) of μ has no derivative, finite or infinite. On the one hand, for the case where p j &gt; a j , Wen xia [<xref ref-type="bibr" rid="scirp.97688-ref5">5</xref>] has been studied the packing and box dimensions of S and give an approach to calculate the Hausdorff dimension of S. Kennen J. Falconer [<xref ref-type="bibr" rid="scirp.97688-ref6">6</xref>] is further noted that Hausdorff dimension of the set of points of non-differentiability of a self-affine “devil’s staircase” function is the square of the dimension of the set of points of increase. On the other hand when r = 2 , for the case where p 1 &lt; a 1 or p 2 &lt; a 2 . Yuanyuan yao, YunXin zhang and wenxia [<xref ref-type="bibr" rid="scirp.97688-ref1">1</xref>] Systematic has been given the Hausdorff and packing dimension of S. Secondly, Reza Mirzaire [<xref ref-type="bibr" rid="scirp.97688-ref7">7</xref>] find an upper bound for the Hausdorff dimension of the nondifferentiability set of a continuous convex function defined on a Riemannian manifold. As an application, he show that the boundary of a convex open subset of R n , n ≥ 2 , has Hausdorff dimension at most n − 2 and David Pavlica [<xref ref-type="bibr" rid="scirp.97688-ref8">8</xref>] characterize sets of non-differentiability points of convex functions on R n . This completes (in R n ) the result by [<xref ref-type="bibr" rid="scirp.97688-ref9">9</xref>] which gives a characterization of the magnitude of these sets. Last, Eidswick [<xref ref-type="bibr" rid="scirp.97688-ref10">10</xref>] points out that the points of nondifferentiability of the Cantor ternary function are characterized in terms of the spacing of 0’s and 2’s in ternary expansions, and have calculated that T μ λ has the cardinality of the continuum.</p><p>Since about the dimension of the set T μ λ of points, Eidswick didn’t study it. So, our main job in this paper is to give its dimension, that is, the following theorem.</p><p>Theorem 1.1. dim H T μ λ = ( log 2 / log 3 ) 2 , and dim P T μ λ = log 2 / log 3 .</p></sec><sec id="s2"><title>2. Proofs of Theorem</title><p>First, we give a proposition, which simplifies the calculation of θ + and θ − .</p><p>Proposition 2.1. Let t = . t 1 t 2 ⋯ t n be ternary expansion of t, and define</p><p>e n = . t 1 t 2 ⋯ t z ( n ) − 1 2 , (2.1)</p><p>d n = . t 1 t 2 ⋯ t z ( n ) − 1 1. (2.2)</p><p>Let</p><p>Q n : = θ ( e n ) − θ ( t ) e n − t     and     P n : = θ ( d n ) − θ ( t ) d n − t ,</p><p>we have</p><p>θ + ( t ) = lim inf n → ∞ Q n , (2.3)</p><p>and</p><p>θ − ( t ) = lim inf n → ∞ P n . (2.4)</p><p>Proof. We just need to prove (2.3), since (2.4) is proved in a similar way.</p><p>If</p><p>lim inf δ → 0 θ ( t + δ ) − θ ( t ) δ = + ∞ ,</p><p>then, the proposition is apparently true.</p><p>So, we suppose that</p><p>lim inf δ → 0 θ ( t + δ ) − θ ( t ) δ = c &lt; + ∞ ,</p><p>then, we can find { δ n } n = 1 + ∞ such that</p><p>lim n → ∞ θ ( t + δ n ) − θ ( t ) δ n = lim inf δ → 0 θ ( t + δ ) − θ ( t ) δ . (2.5)</p><p>Note that e n + 1 + 1 3 Z ( n + 1 ) = d n and lim n → + ∞ d n = t , we have</p><p>( t , e 1 + 1 3 z ( 1 ) ) = ∪ n = 1 + ∞ [ d n , e n + 1 3 z ( n ) )     .</p><p>Therefore, for any k ≥ 1 , there is an integer n k , such that t + δ k ∈ [ d n k , e n k + 1 3 z ( n k ) ) .</p><p>By (2.5), for any ε &gt; 0 , there is an integer N &gt; 0 such that: when k &gt; N ,</p><p>θ ( t + δ k ) − θ ( t ) δ k &lt; c + ε .</p><p>Denote η k = t + δ k − e n k , then 0 &lt; η k &lt; 3 − z ( n k ) , we have</p><p>θ ( t + δ k ) = θ ( e n k + η k ) = θ ( e n k ) + θ ( η k ) .</p><p>So,</p><p>θ ( e n k ) − θ ( t ) e n k − t = θ ( t + δ k ) − θ ( η k ) − θ ( t ) δ k − η k ,</p><p>and since lim k → + ∞ θ ( η k ) η k = + ∞ , it follows that</p><p>lim inf k → + ∞ θ ( e n k ) − θ ( t ) e n k − t ≤ lim k → + ∞ θ ( t + δ k ) − θ ( t ) δ k .</p><p>On the other hand, it is obvious that:</p><p>lim inf k → + ∞ θ ( e n k ) − θ ( t ) e n k − t ≥ lim inf δ → 0 θ ( t + δ ) − θ ( t ) δ ,</p><p>so we complete the proof of (2.3).</p><p>☐</p><p>Besides, we need the following Lemma due to Billingsley:</p><p>Lemma 2.2. Let b ≥ 2 be an integer and for x ∈ [ 0,1 ] , let I n ( x ) be the nth generation half-open b-adic interval of the form [ j − 1 b n , j b n ] cintaining x, let</p><p>A ⊂ [ 0,1 ] be Borel and let μ be a finite Borel measure on [0, 1], suppose μ ( A ) &gt; 0 . If</p><p>α ≤ lim inf n → ∞ log μ ( I n ( x ) ) log | I n ( x ) | ≤ β ,</p><p>then</p><p>α ≤ dim H ( A ) ≤ β .</p><p>For the proof of this lemma, we refer readers to Section 1.4 of [<xref ref-type="bibr" rid="scirp.97688-ref11">11</xref>].</p><p>Corollary 2.3. For S ⊂ N , define</p><p>A S = { x : ∑ k ∈ S     x k 3 k : x k ∈ { 0,2 } } . (2.6)</p><p>We have</p><p>dim H ( A S ) = lim _ N → ∞ # ( S ∩ { 1, ⋯ , N } ) N ⋅ log 2 log 3 . (2.7)</p><p>Proof. To see this, let μ be the probability measure on A S that give equal measure to nth generation covering intervals. This measure makes the digits { x k } k ∈ S in (2.6) independent identically distributed uniform random bits. For any x ∈ A S ,</p><p>log μ ( I n ( x ) ) log | I n ( x ) | = log 2 − # ( S ∩ { 1, ⋯ , N } ) log 3 − n = # ( S ∩ { 1, ⋯ , N } ) N ⋅ log 2 log 3 .</p><p>Thus the liminf of the left-hand side is the liminf of the right-hand side. By Lemma 2.2, this proves the corollary.</p><p>Last, we need to introduce a theorem and a formula:</p><p>Theorem 2.4. Let t be a point of T which is not an endpoint of a comple-mentary interval, let z ( n ) denote the position of the nth zero in its ternary</p><p>expansion, and let λ = lim inf n → ∞ 3 z ( n ) 2 ( n + 1 ) . Then λ ≤ θ + ( t ) ≤ 2 λ . Furthermore, if z ( n + 1 ) − z ( n ) → ∞ , then, θ + ( t ) = λ .</p><p>Let, Q n = θ ( e n ) − θ ( t ) e n − t . Then,</p><p>Q n = 3 z ( n ) 2 z ( n + 1 ) ∑ 1 ∞ 2 − ( z ( n + k ) − z ( n + 1 ) ) 1 + 2 ∑ 1 ∞ 3 − ( z ( n + k ) z ( n ) ) (2.8)</p><p>The proof of theorem 2.4 and formula (2.8), we see [<xref ref-type="bibr" rid="scirp.97688-ref10">10</xref>].</p><p>Proof of Theorem. First, let’s construct a subset of T μ λ .</p><p>Let μ 0 = log μ log 2 , λ 0 = log λ log 2 . We can find increasing sequences of positive integers ( a n ) and ( b n ) such that</p><p>a 2 n ξ − b 2 n → λ 0 , (2.9)</p><p>and</p><p>a 2 n + 1 ξ − b 2 n + 1 → μ 0 , (2.10)</p><p>when n is large enough, where ξ = log 3 log 2 . At the same time, we may request that a n &lt; b n , a n + 1 − b n ≥ 4 n and b n ≥ 3 n hold for all n ≥ 1 . Moreover, denote M = [ a 2 n + 1 − b 2 n 2 n ] and M * = [ a 2 n + 2 − b 2 n + 1 2 n ] , we insert these points ( b 2 n , i ) i = 1 M and ( b 2 n + 1 , j ) j = 1 M * in to ( b 2 n , a 2 n + 1 ) and ( b 2 n + 1 , a 2 n + 2 ) , respectively, such that</p><p>b 2 n , i + 1 − b 2 n , i = 2 n , (2.11)</p><p>and</p><p>b 2 n + 1 , j + 1 − b 2 n + 1 , j = 2 n , (2.12)</p><p>when n is large enough, for i = 1 , 2 , ⋯ , M and j = 1 , 2 , ⋯ , M * ; and let b 2 n = b 2 n , 0 , b 2 n + 1 , 0 = b 2 n + 1 . We will show the selection of { a n } and { b n } later.</p><p>Define t m = 0 , if m ∈ { a 2 n , b 2 n , b 2 n ,1 , ⋯ , b 2 n , M , b 2 n + 1,1 + 1, b 2 n + 1,2 + 1, ⋯ , b 2 n + 1, M * + 1 } , or a 2 n + 1 &lt; m &lt; b 2 n + 1 .</p><p>Define t m = 0 , if m ∈ { a 2 n + 1 , b 2 n + 1 , b 2 n + 1,1 , b 2 n + 1,2 , ⋯ , b 2 n + 1, M * , b 2 n ,1 + 1, b 2 n ,2 + 1, ⋯ , b 2 n , M + 1 } , or a 2 n &lt; m &lt; b 2 n .</p><p>And restrict t m ∈ { 0,2 } (That is, t m is free to take a value of 0 or 2 for all other values of m).</p><p>And we claim that t = ∑ m = 1 ∞ t m 3 m ∈ T μ λ . We’ll give a simple proof after the selection of ( a n ) n = 1 + ∞ and ( b n ) n = 1 + ∞ , let Ω be the set of all such t.</p><p>For the selection of ( a n ) n = 1 + ∞ , ( b n ) n = 1 + ∞ , first of all, take a 0 = b 0 = 1 . Assume that a 2 n and b 2 n is taken, we choose a 2 n + 1 , such that</p><p>(a) a 2 n + 1 ≥ 8 n + b 2 n ;</p><p>(b) [ ξ a 2 n + 1 ] − [ μ 0 ] &gt; a 2 n + 1 (note that ξ &gt; 1 );</p><p>(c) | { ξ a 2 n + 1 } − { μ 0 } | &lt; 1 n (note that ( ξ n ) is uniformly distributed modulo 1).</p><p>where [ x ] represents the integer part that represents taking x, and { y } represents the fractional portion of the y. And take b 2 n + 1 = [ ξ a 2 n + 1 ] − [ μ 0 ] . We choose a 2 n + 2 such that</p><p>(d) a 2 n + 2 ≥ 4 ( 2 n + 1 ) + b 2 n + 1 ;</p><p>(e) [ ξ a 2 n + 2 ] − [ λ 0 ] &gt; a 2 n + 2 ;</p><p>(f) | { ξ a 2 n + 2 } − { λ 0 } | &lt; 1 n + 1 .</p><p>and take b 2 n + 2 = [ ξ a 2 n + 2 ] − [ λ 0 ] .</p><p>These ( a n ) n = 1 + ∞ and ( b n ) n = 1 + ∞ meet the desired conditions.</p><p>From a 2 n ξ − b 2 n → λ 0 and a 2 n + 1 ξ − b 2 n + 1 → μ 0 , we can get that</p><p>3 a 2 n 2 b 2 n → λ     and     3 a 2 n + 1 2 b 2 n + 1 → μ .</p><p>To see that t = ∑ m = 1 ∞ t m 3 m ∈ T μ λ , by the Theorem 2.4 and formula (2.8), we only</p><p>need to show that b 2 n and a 2 n are adjacent positions of zeros, whose spacing is largest; and b 2 n + 1 and a 2 n + 1 are adjacent positions of twos, whose spacing is largest.</p><p>Since a 2 n → b 2 n ξ + λ ξ , for any ϵ &gt; 0 , when n is large enough, we have</p><p>| a 2 n − b 2 n ξ − λ ξ | &lt; ϵ ,</p><p>then, when n is large enough</p><p>b 2 n − a 2 n &gt; b 2 n − b 2 n ξ − λ 0 ξ − ε = ( 1 − 1 ξ ) b 2 n − λ 0 ξ − ε ≈ 0.36 b 2 n &gt; 2 n .</p><p>Then, according to our above-mentioned construction of t = ∑ m = 1 ∞ t m 3 m , other</p><p>spacings of zeros are at most 2n, so b 2 n − a 2 n is the largest spacing of zeros. Similarly, we have b 2 n + 1 − a 2 n + 1 &gt; 2 n , and b 2 n + 1 − a 2 n + 1 is the largest spacing of twos.</p><p>Denote</p><p>A n = ( { k ∈ N : b 2 n ≤ k ≤ a 2 n + 1 } ∪ { k ∈ N : b 2 n + 1 ≤ k ≤ a 2 n + 1 } ) ,</p><p>B n = ( ( ∪ i = 1 M { b 2 n , i , b 2 n , i + 1 } ) ∪ ( ∪ j = 1 M * { b 2 n + 1 , j ,   b 2 n + 1 , j + 1 } ) ) .</p><p>Let</p><p>B : = ∪ n = 1 + ∞ ( A n \ B n )</p><p>in fact, the set B is all positions that t m can freely select 0 or 2 in the above construction. Using Corollary 2.3, we have</p><p>dim p Ω = dim B Ω = lim sup N → ∞ # { k ∈ B , k ≤ N } N ⋅ log 2 log 3 ,</p><p>and</p><p>dim H Ω = lim inf N → ∞ # { k ∈ B , k ≤ N } N ⋅ log 2 log 3 .</p><p>And we calculate these as follows: It’s not hard to see that, when N = a 2 n + 1 , we can get the superior limit:</p><p>lim sup N → ∞ # { k ∈ B , k ≤ N } N ⋅ log 2 log 3 = lim n → ∞ a 2 n + 1 − b 2 n − 2 M a 2 n + 1 ⋅ log 2 log 3 = log 2 log 3</p><p>where lim n → ∞ b 2 n a 2 n + 1 = 0 , lim n → ∞ M a 2 n + 1 = 0 .</p><p>On the other hand, when N = b n , we can get the inferior limit:</p><p>dim H Ω = liminf N → ∞ # { k ∈ B , k ≤ N } N ⋅ log 2 log 3 = lim n → ∞ # { k ∈ B , k ≤ b n } n ⋅ log 2 log 3 ,</p><p>and by calculating</p><p>lim n → ∞ # { k ∈ B , k ≤ b 2 n + 1 } b 2 n + 1 ⋅ log 2 log 3 ≥ lim n → ∞ a 2 n + 1 − b 2 n − 2 M b 2 n + 1 ⋅ log 2 log 3 = ( log 2 / log 3 ) 2</p><p>where lim n → ∞ a 2 n + 1 b 2 n + 1 = log 2 log 3 , lim n → ∞ b 2 n b 2 n + 1 = 0 and lim n → ∞ M b 2 n + 1 = 0 ;</p><p>lim n → ∞ # { k ∈ B , k ≤ b 2 n + 2 } b 2 n + 2 ⋅ log 2 log 3 ≥ lim n → ∞ a 2 n + 2 − b 2 n + 1 − 2 M * b 2 n + 2 ⋅ log 2 log 3 = ( log 2 / log 3 ) 2</p><p>where lim n → ∞ a 2 n + 2 b 2 n + 2 = log 2 log 3 , lim n → ∞ b 2 n + 1 b 2 n + 2 = 0 , lim n → ∞ M * b 2 n + 2 = 0 .</p><p>In Section 1, we already know dim p N * = log 2 / log 3 , and dim H N * = ( log 2 / log 3 ) 2 .</p><p>Since Ω ⊂ T μ λ ⊂ N * , we have dim H Ω = dim H T μ λ = ( log 2 / log 3 ) 2 and dim P Ω = dim P T μ λ = log 2 / log 3 .</p></sec><sec id="s3"><title>3. Conclusion</title><p>Finally, through the above proof, we solved dimension of the set T μ λ of points that is Eidswick didn’t study it. In other words, we finally get that dim H T μ λ = ( log 2 / log 3 ) 2 , and dim P T μ λ = log 2 / log 3 .</p></sec><sec id="s4"><title>Conflicts of Interest</title><p>The author declares no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s5"><title>Cite this paper</title><p>Yan, M.Q. (2020) Dimension of the Non-Differentiability Subset of the Cantor Function. Journal of Applied Mathematics and Physics, 8, 107-114. https://doi.org/10.4236/jamp.2020.81009</p></sec></body><back><ref-list><title>References</title><ref id="scirp.97688-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Yao, Y.Y., Zhang, Y.X. and Li, W.X. (2009) Dimension of Non-Differentiability Points of Cantor Functions. 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