Some Sets of GCF ϵ Expansions Whose Parameter ϵ Fetch the Marginal Value

Similar documents
THE HAUSDORFF MEASURE OF SIERPINSKI CARPETS BASING ON REGULAR PENTAGON

c n b n 0. c k 0 x b n < 1 b k b n = 0. } of integers between 0 and b 1 such that x = b k. b k c k c k

Geometric Measure Theory

TRIPLE SOLUTIONS FOR THE ONE-DIMENSIONAL

MULTIPLE POSITIVE SOLUTIONS OF BOUNDARY VALUE PROBLEMS FOR P-LAPLACIAN IMPULSIVE DYNAMIC EQUATIONS ON TIME SCALES

ON THE APPROXIMATION ERROR IN HIGH DIMENSIONAL MODEL REPRESENTATION. Xiaoqun Wang

New bounds for Morse clusters

Multi-dimensional Fuzzy Euler Approximation

Unbounded solutions of second order discrete BVPs on infinite intervals

arxiv: v2 [math.nt] 30 Apr 2015

SOME RESULTS ON INFINITE POWER TOWERS

A SIMPLE NASH-MOSER IMPLICIT FUNCTION THEOREM IN WEIGHTED BANACH SPACES. Sanghyun Cho

One Class of Splitting Iterative Schemes

arxiv: v1 [math.ca] 23 Sep 2017

arxiv: v1 [math.mg] 25 Aug 2011

Manprit Kaur and Arun Kumar

THE DIVERGENCE-FREE JACOBIAN CONJECTURE IN DIMENSION TWO

SOLUTIONS TO ALGEBRAIC GEOMETRY AND ARITHMETIC CURVES BY QING LIU. I will collect my solutions to some of the exercises in this book in this document.

Chapter 4. The Laplace Transform Method

TAYLOR POLYNOMIALS FOR NABLA DYNAMIC EQUATIONS ON TIME SCALES

Research Article Existence for Nonoscillatory Solutions of Higher-Order Nonlinear Differential Equations

(3) A bilinear map B : S(R n ) S(R m ) B is continuous (for the product topology) if and only if there exist C, N and M such that

OSCILLATIONS OF A CLASS OF EQUATIONS AND INEQUALITIES OF FOURTH ORDER * Zornitza A. Petrova

CHAPTER 4 DESIGN OF STATE FEEDBACK CONTROLLERS AND STATE OBSERVERS USING REDUCED ORDER MODEL

Optimal Strategies for Utility from Terminal Wealth with General Bid and Ask Prices

Beta Burr XII OR Five Parameter Beta Lomax Distribution: Remarks and Characterizations

Multicolor Sunflowers

Theoretical Computer Science. Optimal algorithms for online scheduling with bounded rearrangement at the end

Component-by-Component Construction of Low-Discrepancy Point Sets of Small Size

SOME MONOTONICITY PROPERTIES AND INEQUALITIES FOR

THE SPLITTING SUBSPACE CONJECTURE

STABILITY OF A LINEAR INTEGRO-DIFFERENTIAL EQUATION OF FIRST ORDER WITH VARIABLE DELAYS

Preemptive scheduling on a small number of hierarchical machines

The fractional stochastic heat equation on the circle: Time regularity and potential theory

General System of Nonconvex Variational Inequalities and Parallel Projection Method

NULL HELIX AND k-type NULL SLANT HELICES IN E 4 1

QUENCHED LARGE DEVIATION FOR SUPER-BROWNIAN MOTION WITH RANDOM IMMIGRATION

arxiv: v1 [math.ac] 30 Nov 2012

CHAPTER 8 OBSERVER BASED REDUCED ORDER CONTROLLER DESIGN FOR LARGE SCALE LINEAR DISCRETE-TIME CONTROL SYSTEMS

A note on the bounds of the error of Gauss Turán-type quadratures

Primitive Digraphs with the Largest Scrambling Index

List coloring hypergraphs

FOURIER SERIES AND PERIODIC SOLUTIONS OF DIFFERENTIAL EQUATIONS

Representation Formulas of Curves in a Two- and Three-Dimensional Lightlike Cone

Stochastic Optimization with Inequality Constraints Using Simultaneous Perturbations and Penalty Functions

A Short Note on Hysteresis and Odd Harmonics

ON A CERTAIN FAMILY OF QUARTIC THUE EQUATIONS WITH THREE PARAMETERS

UNIQUE CONTINUATION FOR A QUASILINEAR ELLIPTIC EQUATION IN THE PLANE

1. Preliminaries. In [8] the following odd looking integral evaluation is obtained.

Convergence criteria and optimization techniques for beam moments

RELIABILITY OF REPAIRABLE k out of n: F SYSTEM HAVING DISCRETE REPAIR AND FAILURE TIMES DISTRIBUTIONS

Lecture 17: Analytic Functions and Integrals (See Chapter 14 in Boas)

STOCHASTIC EVOLUTION EQUATIONS WITH RANDOM GENERATORS. By Jorge A. León 1 and David Nualart 2 CINVESTAV-IPN and Universitat de Barcelona

Strong Stochastic Stability for MANET Mobility Models

Avoiding Forbidden Submatrices by Row Deletions

Spacelike Salkowski and anti-salkowski Curves With a Spacelike Principal Normal in Minkowski 3-Space

Lecture 8: Period Finding: Simon s Problem over Z N

ON A CERTAIN FAMILY OF QUARTIC THUE EQUATIONS WITH THREE PARAMETERS. Volker Ziegler Technische Universität Graz, Austria

Introduction to Laplace Transform Techniques in Circuit Analysis

Computers and Mathematics with Applications. Sharp algebraic periodicity conditions for linear higher order

P ( N m=na c m) (σ-additivity) exp{ P (A m )} (1 x e x for x 0) m=n P (A m ) 0

New index matrix representations of operations over natural numbers

INITIAL VALUE PROBLEMS OF FRACTIONAL ORDER HADAMARD-TYPE FUNCTIONAL DIFFERENTIAL EQUATIONS

Lecture 9: Shor s Algorithm

Reliability Analysis of Embedded System with Different Modes of Failure Emphasizing Reboot Delay

7.2 INVERSE TRANSFORMS AND TRANSFORMS OF DERIVATIVES 281

Given the following circuit with unknown initial capacitor voltage v(0): X(s) Immediately, we know that the transfer function H(s) is

A relationship between generalized Davenport-Schinzel sequences and interval chains

arxiv: v4 [math.co] 21 Sep 2014

ENGEL SERIES EXPANSIONS OF LAURENT SERIES AND HAUSDORFF DIMENSIONS

Math 273 Solutions to Review Problems for Exam 1

REVERSE HÖLDER INEQUALITIES AND INTERPOLATION

Flag-transitive non-symmetric 2-designs with (r, λ) = 1 and alternating socle

Optimal Coordination of Samples in Business Surveys

Robustness analysis for the boundary control of the string equation

COHOMOLOGY AS A LOCAL-TO-GLOBAL BRIDGE

Convex Hulls of Curves Sam Burton

ON THE SMOOTHNESS OF SOLUTIONS TO A SPECIAL NEUMANN PROBLEM ON NONSMOOTH DOMAINS

Lecture 10 Filtering: Applied Concepts

Moment of Inertia of an Equilateral Triangle with Pivot at one Vertex

Weber Schafheitlin-type integrals with exponent 1

February 5, :53 WSPC/INSTRUCTION FILE Mild solution for quasilinear pde

A CATEGORICAL CONSTRUCTION OF MINIMAL MODEL

Approximate Analytical Solution for Quadratic Riccati Differential Equation

Social Studies 201 Notes for November 14, 2003

Reformulation of Block Implicit Linear Multistep Method into Runge Kutta Type Method for Initial Value Problem

A PROOF OF TWO CONJECTURES RELATED TO THE ERDÖS-DEBRUNNER INEQUALITY

Bogoliubov Transformation in Classical Mechanics

By Xiaoquan Wen and Matthew Stephens University of Michigan and University of Chicago

On the Unit Groups of a Class of Total Quotient Rings of Characteristic p k with k 3

Lecture 2 - Geometric Convergence

Social Studies 201 Notes for March 18, 2005

NUMBERS. := p n 1 + p n 2 q + p n 3 q pq n 2 + q n 1 = pn q n p q. We can write easily that [n] p,q. , where [n] q/p

A Simplified Methodology for the Synthesis of Adaptive Flight Control Systems

UNIT 15 RELIABILITY EVALUATION OF k-out-of-n AND STANDBY SYSTEMS

SMALL-SIGNAL STABILITY ASSESSMENT OF THE EUROPEAN POWER SYSTEM BASED ON ADVANCED NEURAL NETWORK METHOD

EFFECTS OF SOIL LAYER CONSTRUCTION ON CHARACTERISTIC PERIODS OF RESPONSE SPECTRA

Local Fractional Laplace s Transform Based Local Fractional Calculus

Research Article Triple Positive Solutions of a Nonlocal Boundary Value Problem for Singular Differential Equations with p-laplacian

Pacific Journal of Mathematics

Transcription:

Journal of Mathematical Reearch with Application May, 205, Vol 35, No 3, pp 256 262 DOI:03770/jin:2095-26520503002 Http://jmredluteducn Some Set of GCF ϵ Expanion Whoe Parameter ϵ Fetch the Marginal Value Liang TANG, Peijuan ZHOU, Ting ZHONG Department of Mathematic, Jihou Univerity, Hunan 427000, P R China Abtract Let ϵ : N R be a parameter function atifying the condition ϵ) + + > 0 and let T ϵ : 0, ] 0, ] be a tranformation defined by T ϵ x) = + + )x + ϵx for x +, ] Under the algorithm T ϵ, every x 0, ] i attached an expanion, called generalized continued fraction GCF ϵ ) expanion with parameter by Schweiger Define the equence { n x)} n of the partial quotient of x by x) = /x and n x) = Tϵ n x)) for every n 2 Under the retriction < ϵ) <, define the et of non-recurring GCF ϵ expanion a F ϵ = {x 0, ] : n+x) > nx) for infinitely many n} It ha been proved by Schweiger that F ϵ ha Lebegue meaure 0 In the preent paper, we trengthen thi reult by howing that { dimh F ϵ, when ϵ) = + ρ for a contant 0 < ρ < ; 2 dim +2 H F ϵ, when ϵ) = + for any where dim H denote the Haudorff dimenion Keyword GCF ϵ expanion; metric propertie; Haudorff dimenion MR200) Subject Claification K55; 28A80 Introduction In 2003, Schweiger [] introduced a new cla of continued fraction with parameter, called generalized continued fraction GCF ϵ ), which are induced by the tranformation T ϵ : 0, ] 0, ] T ϵ x) := where the parameter ϵ : N R atifie + + )x + ϵ ϵx when x +, ] =: B) ) ϵ) + + > 0, for all 2) Received July 24, 204; Accepted December 22, 204 Supported by the National Natural Science Foundation of China Grant No 36025) * Correponding author E-mail addre: tl3022@26com Liang TANG); peijuanzhou@26com Peijuan ZHOU); zhongting 2005@26 com Ting ZHONG)

Some et of GCF ϵ expanion whoe parameter ϵ fetch the marginal value 257 For any x 0, ], it partial quotient { n } n in the GCF ϵ expanion are defined a = x) :=, and n = n x) := T n ϵ x) x ) By the algorithm ), it follow [] that x = A n + B n T n ϵ x) C n + D n T n ϵ x) for all n, where the number A n, B n, C n, D n are given by the recurive relation ) ) C n D n C n D n n + n ϵ n ) = A n B n C n B n + ϵ n ) ) ) C 0 D 0 0 with = A 0 B 0 0 ) n, 3) A well own example of the generalized continued fraction i in the cae that the parameter function ϵ 0 In thi cae, the algorithm ) become T x) = + + )x when x +, ] Then every x 0, ] can be expanded into a erie with the form x = x) + + + + ) 2 x) + ) n x) + ) + Actually thi i the Engel erie expanion which wa well tudied in the literature, ee Erdö, Rényi & Szüz [2], Rényi [3], Galambo [4] and Liu, Wu [5], etc Schweiger [] tudied the arithmetical a well a the ergodic propertie of GCF ϵ map At the ame time, he howed that with different choice of the parameter function ϵ, the tochatic propertie of the partial quotient differ greatly Concerning the propertie of the partial quotient, by the condition hared by the parameter ϵ) ee 2)), it i clear that n+ x) n x) for all n, ie, the partial quotient equence of x i non-decreaing We invetigated the metrical propertie of { n } n further in [8] and proved that when < ϵ), for almot all x 0, ], log n x) lim =, n and when ϵ) =, thi equality i no longer true It wa alo hown [7] that the partial quotient in the GCF ϵ expanion hare a 0- law and the central limit theorem under the retriction of < ϵ) Thee reult howed that when < ϵ), the metric propertie of GCF ϵ and Engel erie expanion are very imilar However, in thi paper we will ee that the ituation change radically when < ϵ) < ρ for a contant 0 < ρ < Thi i becaue in thi cae, T ϵ ha two fixed point ϵ and in every interval B) := +, ] So all B) can be divided into two ubinterval a: [ B ) =: +, ] and B + ) =: ϵ) ϵ), ]

258 Liang TANG, Peijuan ZHOU and Ting ZHONG uch that T B + ) = B + ) Therefore if, 2,, n, + ) i an admiible bloc, then n < And it i eay to ee that, the et defined by F ϵ = B, 2,, n ) 4) n= n i a complementary et of the ultimately recurring GCF ϵ expanion That i F ϵ := {x 0, ] : n+ x) > n x) for infinitely many n} We define the cylinder et a follow For any non-decreaing integer vector,, n ), define the n-th order cylinder a follow B,, n ) = {x 0, ] : j x) = j, j n} an nth order cylinder, which i the et of point whoe partial quotient begin with,, n ) Then the following reult have been obtained in ection 3 of []: B, 2,, n ) = B nc n A n D n C n n C n + D n ) ; 5) B, 2,, n ) B n C n A n D n = C n ϵ n )C n + D n ) ; 6) λ ) ) F ϵ = λ B, 2,, n ) = 0, 7) n= < < n where < ϵ) < + ρ for a contant 0 < ρ < In thi paper, we trengthen the reult 7) by howing that Theorem Let F ϵ be the et defined above Then { dim H F ϵ 2, when ϵ) = + ρ for a contant 0 < ρ < ; +2 dim H F ϵ, when ϵ) = + for any where dim H denote the Haudorff dimenion 2 Preliminary later ue In thi ection, we preent ome imple fact about the generalized continued fraction for The firt lemma concern the relationhip between A n, B n, C n, D n which are recurively defined by 3) Lemma 2 [,8]) For all n, i) C n = n + )C n + D n > 0; ii) D n = n ϵ n )C n + + ϵ n ))D n, and D n 0 when ϵ 0; D n < 0 when ϵ < 0; iii) n C n + D n = n C n + D n ) n + + ϵ n )); iv) B n C n A n D n = B N C N A N D N ) n i=n+ i + + ϵ i )) > 0, 0 N < n The following lemma are epecially aimed for ϵ) = +

Some et of GCF ϵ expanion whoe parameter ϵ fetch the marginal value 259 Lemma 22 If ϵ) = +, then when n 2, n C n + D n = nc n + D n n > 0; ϵ n )C n + D n C n 2 Proof By Lemma 2 iii) and the condition ϵ) = +, noticing that n n, we have n C n + D n = nc n + D n n Thi alo give that Uing Lemma 2 i) and 8), we get n C n + D n n C + D n n 2 > 0 D n n C n 8) C n n + )C n n C n n + n )C n C n C = + 2 Thu C n 2 i proved Uing 8) again, we can find that when n 2, ϵ n )C n + D n n + )C n n C n = )C n 2 C n The next lemma will be ued for etimating the lower bound of dim H F ϵ Lemma 23 [,8]) Let ϵ) = + Then when n 2, C n + D n 0; n C n + D n ϵ n )C n + D n C n n n Proof By Lemma 2 i) ii), we have C n + D n = n + )C n + D n + n n + )C n + n + )D n = C n + D n + n + ) n C n + D n ) Then by Lemma 2 i), we have Thu n C n + D n n C n + D n ) 0 C n = n C n + C n + D n ) n C n n n 9) By the condition ϵ) = +, we have, n < ϵ n ) = n + n C n + D n ϵ n )C n + D n = n C n + D n ) + )C n 0) Then uing the firt equality of Lemma 22, we get ϵ n )C n + D n = nc n + D n n So the econd reult follow from 0), ) and 9) + )C n = C n C n C n )

260 Liang TANG, Peijuan ZHOU and Ting ZHONG Now we focu on the propertie of the point et F ϵ with ϵ) = + for any n From now on until the end of thi paper, we fix a point x F ϵ and let n = n x) be the nth partial quotient of x The number A n, B n, C n, D n are recurively defined by 3) for x 3 The Haudorff dimenion of E ϵ α) The proof of Theorem i divided into two part: one for upper bound, the other for lower bound 3 Upper bound Fix δ > 0 Since n = that for all j M, ) +δ = n= n= j n n +δ ) +δ converge, there exit M large enough o 2) From 4), we can ee that n B, 2,, n ) i a natural covering of F ϵ for any n Then the +δ -dimenional Haudorff meaure of F ϵ can be etimated a H +δ Fϵ ) lim inf i+ i i n B, 2,, n ) Under the condition ϵ) = +, by Lemma 2 iv), we have B n C n A n D n = +δ 2 n ) 3) On the other hand, by Lemma 22, we have C n ϵ n )C n + D n ) 2 Then uing 6), we get B, 2,, B n C n A n D n n ) = C n ϵ n )C n + D n ) 2 2 n ) 2 2 N ) N+ N+2 Thu by 2), we have H +δ Fϵ ) lim inf lim inf lim inf i+ i i N i+ i i N i+ i i n B, 2,, n ) ) +δ 2 N ) N+ N ) +δ 2 N ) < +δ N+ ) +δ n n which give that dim H E ϵ α) +δ Since thi i true for all δ > 0, we get dim H E ϵ α) for ϵ) = + and any n ) +δ

Some et of GCF ϵ expanion whoe parameter ϵ fetch the marginal value 26 32 Lower bound In order to etimate the lower bound, we recall the claical dimenional reult concerning a pecially defined Cantor et Lemma 3 [6]) Let I = E 0 E E 2 be a decreaing equence of et, with each E n, a union of a finite number of dijoint cloed interval If each interval of E n contain at leat m n interval of E n n =, 2, ) which are eparated by gap of at leat η n, where 0 < η n+ < η n for each n Then the lower bound of the Haudorff dimenion of E can be given by the following inequality: dim H n E n ) lim inf logm m 2 m n ) logm n η n ) Now for each n, let E = {x 0, ] : 2 n < n x) < 2 n+, n } Clearly, if x E, then n x) > n x) for all n Thi implie that E F ϵ For each n, let E n be the collection of cylinder E n = {B n,, n ) : 2 i < i x) < 2 i+, i n} 4) Then E = n= E n, and E fulfill the contruction of the Cantor et in Lemma 3 Now we pecify the integer {m n, n } and the real number {η n, n } E n, and Due to the definition of E n, each interval of E n contain m n = 2 n 2 n interval of m m 2 m n = 2 +2+ +n 2) = 2 n 2)n ) 2 ; 5) and any two of interval in E n are eparated by at leat one interval B,, n, + n ) By 5) and 6), we have B,, n, + n ) = B,, n, n ) B,, n, n ) = B nc n A n D n C n n C n + D n ) B n C n A n D n C n ϵ n )C n + D n ) = B nc n A n D n ) ϵ n ) n ) n C n + D n ) ϵ n )C n + D n ) By Lemma 23 and the equality 3), the above equality give that B,, n, + n ) 2 n ) +2 In view of 4), the partial quotient n atify that 2 n < n x) < 2 n+ for all n Therefore, B,, n, + n ) A a reult of 5) and 6), we get lim inf 2 2+3+ +n+) ) = +2 2 nn+)+2) 2 log 2 m m n ) log 2 m n η n ) = + 2 Combining thi with Lemma 3, we get when ϵ) = + for any, dim H F ϵ dim H E + 2 =: η 6)

262 Liang TANG, Peijuan ZHOU and Ting ZHONG Uing the ame method of proof, we can get dim H F ϵ 2 contant 0 < ρ < when ϵ) = + ρ for a Acowledgement We than the referee for their time and comment Reference [] F SCHWEIGER Continued fraction with increaing digit Öterreich Aad Wi Math-Natur Kl Sitzungber II, 2003, 22: 69 77 [2] P ERDÖS, A RÉNYI, P SZÜSZ On Engel and Sylveter erie Ann Univ Sci Budapet Eötvö Sect Math, 958, : 7 32 [3] A RÉNYI A new approach to the theory of Engel erie Ann Univ Sci Budapet Eötvö Sect Math, 962, 5: 25 32 [4] J GALAMBOS Reprentation of Real Number by Infinite Serie Lecture Note in Math Vol502, Berlin, Springer, 976 [5] Yanyan LIU, Jun WU Some exceptional et in Engel expanion Nonlinearity, 2003, 62): 559 566 [6] K J FALCONER Fractal Geometry Mathematical Foundation and Application Wiley, 990 [7] Luming SHEN, Yuyuan ZHOU Some metric propertie on the GCF fraction expanion J Number Theory, 200, 30): 9 [8] Ting ZHONG Metrical propertie for a cla of continued fraction with increaing digit J Number Theory, 2008, 286): 506 55