Hindawi Publishing Corporation Journal of Probability and Statistics Volume 2016, Article ID 5862107, 10 pages http://dx.doi.org/10.1155/2016/5862107 Research Article Cesàro Summable Sequence Spaces over the Non-Newtonian Complex Field ULur Kadak Department of Mathematics, Faculty of Sciences and Arts, Bozok University, Turkey Correspondence should be addressed to UgΜur Kadak; [email protected] Received 12 September 2015; Accepted 27 October 2015 Academic Editor: Chin-Shang Li Copyright © 2016 UgΜur Kadak. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. π π can be considered the sets of all sequences that are strongly summable to zero, strongly summable, The spaces π0 , ππ , and πβ and bounded, by the CesaΜro method of order 1 with index π. Here we define the sets of sequences which are related to strong CesaΜro summability over the non-Newtonian complex field by using two generator functions. Also we determine the π½-duals of the new spaces and characterize matrix transformations on them into the sets of β-bounded, β-convergent, and β-null sequences of non-Newtonian complex numbers. 1. Introduction The theory of sequence spaces is the fundamental of summability. Summability is a wide field of mathematics, mainly in analysis and functional analysis, and has many applications, for instance, in numerical analysis to speed up the rate of convergence, in operator theory, the theory of orthogonal series, and approximation theory. Also, the concepts of statistical convergence have been studied by various mathematicians. In recent years, generalizations of statistical convergence have appeared in the study of strong integral summability and the structure of ideals of bounded continuous functions on locally compact spaces. Many important sequence spaces arise in a natural way from different notions of summability, that is, ordinary, absolute, and strong summability. The first two cases may be considered as the domains of the matrices that define the respective methods; the situation, however, is different and more complicated in the case of strong summability. Many authors have extensively developed the theory of the matrix transformations between some sequence spaces; we refer the reader to [1β6]. As an alternative to the classical calculus, Grossman and Katz [7β9] introduced the non-Newtonian calculus consisting of the branches of geometric, quadratic, and harmonic calculus, and so forth. All these calculi can be described simultaneously within the framework of a general theory. They decided to use the adjective non-Newtonian to indicate any of calculi other than the classical calculus. Every property in classical calculus has an analogue in non-Newtonian calculus which is a methodology that allows one to have a different look at problems which can be investigated via calculus. In some cases, for example, for wage-rate (in dollars, euro, etc.) related problems, the use of bigeometric calculus which is a kind of non-Newtonian calculus is advocated instead of a traditional Newtonian one. Many authors have extensively developed the notion of multiplicative calculus; see [10β12] for details. Also some authors have also worked on the classical sequence spaces and related topics by using non-Newtonian calculus [13β15]. Further Kadak [16] and Kadak et al. [17, 18] have matrix transformations between certain sequence spaces over the non-Newtonian complex field and have generalized RungeKutta method with respect to the non-Newtonian calculus. The main focus of this work is to extend the strong CesaΜro summable sequence spaces defined earlier to their generalized sequence spaces over the non-Newtonian complex field by using various generator functions, that is, exp and ππ generators. 2. Preliminaries, Background, and Notations Arithmetic is any system that satisfies the whole of the ordered field axioms whose domain is a subset of R. There 2 Journal of Probability and Statistics are infinitely many types of arithmetic, all of which are isomorphic, that is, structurally equivalent. A generator is a one-to-one function whose domain is R and whose range is a subset RπΌ of R where RπΌ = {πΌ(π₯) : π₯ β R}. Each generator generates exactly one arithmetic, and conversely each arithmetic is generated by exactly one generator. If πΌ(π₯) = π₯ for all π₯ β R, then πΌ is called identity function whose inverse is itself. In the special cases πΌ = πΌ and πΌ = exp, πΌ generates the classical and geometric arithmetic, respectively. By πΌ-arithmetic, we mean the arithmetic whose domain is R and whose operations are defined as follows. For π₯, π¦ β RπΌ and any generator πΌ, . β1 β1 πΌ-addition π₯ + π¦ = πΌ {πΌ (π₯) + πΌ (π¦)} . πΌ-subtraction π₯ β π¦ = πΌ {πΌβ1 (π₯) β πΌβ1 (π¦)} . πΌ-multiplication π₯ × π¦ = πΌ {πΌβ1 (π₯) × πΌβ1 (π¦)} . β1 (1) β1 πΌ-division π₯ / π¦ = πΌ {πΌ (π₯) ÷ πΌ (π¦)} . πΌ-order π₯ < π¦ ββ πΌβ1 (π₯) < πΌβ1 (π¦) . As an example if we choose exp function from R to the set Rexp β R+ , πΌ : R σ³¨β Rexp π₯ σ³¨σ³¨β π¦ = πΌ (π₯) = ππ₯ , (2) . π π=1 π=1 β1 = πΌ {πΌ (π₯1 ) + β β β + πΌ (π₯π )} Definition 1 (see [13]). Let π = (π, ππΌ ) be an πΌ-metric space. Then the basic notions can be defined as follows: (a) A sequence π₯ = (π₯π ) is a function from the set N into the set RπΌ . The πΌ-real number π₯π denotes the value of the function at π β N and is called the πth term of the sequence. (b) A sequence (π₯π ) in π = (π, ππΌ ) is said to be πΌ. . convergent if, for every given π > 0 (π β RπΌ ), there exist π0 = π0 (π) β N and π₯ β π such that . . ππΌ (π₯π , π₯) = |π₯π β π₯|πΌ < π for all π > π0 and is denoted πΌ by πΌ limπββ π₯π = π₯ or π₯π σ³¨ β π₯, as π β β. (c) A sequence (π₯π ) in π = (π, ππΌ ) is said to be πΌ-Cauchy . . if for every π > 0 there is π0 = π0 (π) β N such that . ππΌ (π₯π , π₯π ) < π for all π, π > π0 . 2 . . π₯3πΌ = π₯2πΌ × π₯ = πΌ {πΌβ1 {πΌ [πΌβ1 (π₯) × πΌβ1 (π₯)]} × πΌβ1 (π₯)} (3) 3 = πΌ {[πΌβ1 (π₯)] } (6) .. . . πΌ-division π₯ / π¦ = π{ln π₯/ ln π¦} = π₯1/ ln π¦ . . π π₯ππΌ = π₯(πβ1)πΌ × π₯ = πΌ {[πΌβ1 (π₯)] } , Following Grosmann and Katz [8] we give the infinitely many ππ -arithmetic, of which the quadratic arithmetic and harmonic arithmetic are special cases for π = 2 and π = β1, respectively. The function ππ : R β Rπ β R and its inverse ππβ1 (π₯) are defined as follows: 1/π π₯>0 {π₯ , { ππ (π₯) = {0, π₯=0 { 1/π , π₯ < 0, β (βπ₯) { π π₯>0 {π₯ , { = (π₯) {0, π₯ = 0, { π , π₯ < 0, β (βπ₯) { βπ₯π β RπΌ . π₯2πΌ = π₯ × π₯ = πΌ {πΌβ1 (π₯) × πΌβ1 (π₯)} = πΌ {[πΌβ1 (π₯)] } πΌ-subtraction π₯ β π¦ = π{ln π₯βln π¦} = π₯ ÷ π¦ ππβ1 (5) β1 . πΌ-addition π₯ + π¦ = π{ln π₯+ln π¦} = π₯ β π¦ . π β π₯π = πΌ { β πΌβ1 (π₯π )} πΌ Throughout this paper, we define the πth πΌ-exponent π₯ππΌ and πth πΌ-root π₯(1/π)πΌ of π₯ β RπΌ by and πΌ-arithmetic turns out to be Geometric arithmetic: πΌ-multiplication π₯ × π¦ = π{ln π₯ ln π¦} = π₯lnπ¦ = π¦lnπ₯ One can easily conclude that the πΌ-summation can be written as follows: (4) (π β R \ {0}) . If π = 1 then the ππ -calculus is reduced to the classical calculus. πΌ and βπ₯ = π₯(1/2)πΌ = π¦ provided there exists π¦ β RπΌ such that 2πΌ π¦ = π₯. 2.1. β-Arithmetic. Suppose that πΌ and π½ be two arbitrarily selected generators and βstar-β also be the ordered pair of types of arithmetic (π½-arithmetic, πΌ-arithmetic). . .. .. .. .. . . . The sets (Rπ½ , + , β , × , / ) and (RπΌ , + , β , × , / ) are complete ordered fields and πππ‘π(πππβπ)-generator generates πππ‘π(πππβπ)-arithmetic, respectively. Definitions given for π½arithmetic are also valid for πΌ-arithmetic. Also πΌ-arithmetic is used for arguments and π½-arithmetic is used for values; in particular, changes in arguments and values are measured by πΌ-differences and π½-differences, respectively. Definition 2 (see [15]). (a) The β-limit of a function π, denoted by β limπ₯βπ π(π₯) = π, at an element π in RπΌ is, if it exists, the unique number π in Rπ½ such that Journal of Probability and Statistics β 3 .. .. . . .. σ΅¨ .. σ΅¨ lim π (π₯) = π ββ βπ > 0 , βπΏ > 0 β σ΅¨σ΅¨σ΅¨σ΅¨π (π₯) β πσ΅¨σ΅¨σ΅¨σ΅¨π½ < π π₯βπ A function π is β-continuous at a point π in RπΌ if and only if π is an argument of π and β limπ₯βπ π(π₯) = π(π). When πΌ and π½ are the identity function πΌ, the concepts of β-limit and β-continuity are identical with those of classical limit and classical continuity. (b) The isomorphism from πΌ-arithmetic to π½-arithmetic is the unique function π (iota) which has the following three properties: (i) π is one to one. . .. . .. . .. π (π’ + V) = π (π’) + π (V) ; π (π’ × V) = π (π’) × π (V) ; (8) .. π (π’ / V) = π (π’) / π (V) ; .. . 2.2. Non-Newtonian Complex Field and Some Inequalities. . . . . .. .. .. .. Let π β (RπΌ , + , β , × , / ) and π β (Rπ½ , + , β , × , / ) be arbitrarily chosen elements from corresponding arithmetic. Then the ordered pair (π, π) β RπΌ × Rπ½ β R2 is called a βpoint. The set of all β-points is called the set of β-complex numbers and is denoted by Cβ ; that is, β C fl {π§ = (π, π) | π β RπΌ , π β Rπ½ } . (9) Define the binary operations addition (β) and multiplication (β) of β-complex numbers π§1β = (π1 , π1 ) and π§2β = (π2 , π2 ): .. = (π1 + π2 , π1 + π2 ) = (πΌ {πΌβ1 (π1 ) + πΌβ1 (π2 )} , π½ {π½β1 (π1 ) + π½β1 π2 }) β β : C × C σ³¨β C .. Then the pair (π, πβ ) and πβ are called a non-Newtonian metric (β-metric) space and a β-metric on π, respectively. The β-distance πβ between two arbitrarily elements π§1β = (π1 , π1 ) and π§2β = (π2 , π2 ) of the set Cβ is defined by πβ (π§1β , π§2β ) . = β [π (π1 β π2 )] π½ 2π½ .. .. 2π½ + (π1 β π2 ) (11) 2 2 = π½ {β[πΌβ1 (π1 ) β πΌβ1 (π2 )] + [π½β1 (π1 ) β π½β1 (π2 )] } . Up to now, we know that Cβ is a field and the distance between two points in Cβ is computed by the function πβ . Let π§β = (π, π) β Cβ be an arbitrary element. The distance function πβ (π§β , 0β ) is called β-norm of π§β and is denoted by .. .. . .. β β β . In other words, let 0β = ( 0 , 0 ) β Cβ ; then .. 2 2 β π§β β = πβ (π§β , 0β ) = π½ {β(πΌβ1 {π}) + (π½β1 {π}) } . (π§1β , π§2β ) σ³¨σ³¨β β .. (NM1) πβ (π₯, π¦) = 0 if and only if π₯ = π¦, .. β : Cβ × Cβ σ³¨β Cβ β for all π1 , π2 β RπΌ and π1 , π2 β Rπ½ . .. It turns out.. that π(π₯) = π½{πΌ (π₯)} for every π₯ in RπΌ and . . that π( π ) = π for every πΌ-integer π. Since, for example, . .. π’ + V = πβ1 {π(π’) + π(V)}, it should be clear that any statement in πΌ-arithmetic can readily be transformed into a statement in π½-arithmetic. β (10) (NM3) πβ (π₯, π¦) β€ πβ (π₯, π§) + πβ (π§, π¦). β1 . π½ {πΌβ1 (π1 ) π½β1 (π2 ) + π½β1 (π1 ) πΌβ1 (π2 )}) (NM2) πβ (π₯, π¦) = πβ (π¦, π₯), V =ΜΈ 0 ; π’ β€ V ββ π (π’) β€ π (V) . π§2β π§1β β π§2β = (πΌ {πΌβ1 (π1 ) πΌβ1 (π2 ) β π½β1 (π1 ) π½β1 (π2 )} , Definition 4. Let π be a nonempty set and let πβ : π × π β Rπ½ be a function such that, for all π₯, π¦, π§ β π, the following axioms hold: π (π’ β V) = π (π’) β π (V) ; π§1β (π§1β , π§2β ) σ³¨σ³¨β Following Grossman and Katz [8] we can give the definition of β-distance and some applications with respect to the β-calculus. (iii) For any numbers π’, V β RπΌ , β (7) Theorem 3 (see [15]). (Cβ , β, β) is a field. (ii) π is from RπΌ onto Rπ½ . . σ΅¨ . σ΅¨ . βπ β Rπ½ , σ΅¨σ΅¨σ΅¨σ΅¨π₯ β πσ΅¨σ΅¨σ΅¨σ΅¨πΌ < πΏ for π₯, πΏ β RπΌ . .. (12) .. Moreover, for all π§1β , π§2β β Cβ we have πβ (π§1β , π§2β ) = β π§1β βπ§2β β .. .. where πβ is the induced metric from β β β norm. Theorem 5 (see [15]). (Cβ , πβ ) is a complete metric space, where πβ is defined by (11). 4 Journal of Probability and Statistics Corollary 6 (see [15]). Cβ is a Banach space with the β-norm .. .. β β β which is defined by (12). Definition 7. (a) Given a sequence π§πβ = (ππ , ππ ) of β-complex numbers, the formal notation β (ii) Let πΌ and π½ be the same generators. Then π§1β .. β π§β = (π1 , π1 ) β (π1 , β π1 ) 2 π=0 π=0 π=0 π΅β (π₯0 ; π) = {π₯ β π | πβ (π₯, π₯0 ) < π} , = (πΌ β ππ , π½ β ππ ) .. π΅β [π₯0 ; π] = {π₯ β π | πβ (π₯, π₯0 ) β€ π} is called an infinite series with β-complex terms, or simply complex β-series for all π β N. Also, for integers π β N, the finite β-sums π πβ = ββππ=0 π§πβ are called the partial sums of complex β-series. If the sequence β-converges to a complex number π β then we say that the series β-converges and write β β π β = βββ π=0 π§π . The number π is then called the β-sum of this series. If (π π ) β-diverges, we say that the series β-diverges or that it is β-divergent. β (b) A β-series βββ π=0 π§π is said to β-converge absolutely if .. .. β β ββπ=0 β π§π β = β for some number β β Rπ½ . (c) Let {ππ (π₯)} be a sequence of functions from π΄ β R to Cβ for each π. We say that {ππ (π₯)} is uniformly β-convergent to π on π΄ if and only if, for each π₯ β π΄ and for an arbitrary .. .. π > 0 (π β Rπ½ ), there exists an integer π = π(π, π₯) such that .. πβ (ππ (π₯), π(π₯)) < π whenever π > π. be uniformly β(d) The series βββ π=0 ππ (π₯) is said to .. .. convergent to π(π₯) on π΄ if, given any π > 0 , there exists an integer π0 (π) such that π .. πβ (β β ππ (π₯) , π (π₯)) < π whenever π β₯ π0 (π) . π=0 (14) π .. .. ππ½ (1/π)π½ π=0 .. π .. .. ππ½ (1/π)π½ β€ (π½ β β π§πβ β ) π=0 .. π .. .. ππ½ + (π½ β β π‘πβ β ) (15) (1/π)π½ . π=0 Remark 9. Let π§1β = (π1 , π1 ), π§2β = (π2 , π2 ) β Cβ . Then the following statements hold: (i) One has π§1β β π§2β = (π1 , π1 ) β (π2 , π2 ) = (πΌ { π½{ πΌβ1 (π1 ) πΌβ1 (π2 ) + π½β1 (π1 ) π½β1 (π2 ) 2 (πΌβ1 (π2 )) + (π½β1 (π2 )) 2 π½β1 (π1 ) πΌβ1 (π2 ) β πΌβ1 (π1 ) π½β1 (π2 ) (πΌβ1 2 (π2 )) + (π½β1 2 (π2 )) (17) }, (16) (18) are β-neighborhood (or β-open (closed) ball) of centre π₯0 and radius π, respectively. We see that an β-open ball of radius π is the set of all points in π whose beta-distance from the center of the ball is less than π and we say directly from the definition that every βneighborhood of π₯0 contains π₯0 ; in other words, π₯0 is a point of each of its β-neighborhoods. Definition 11. Let (π, πβ ) be a β-metric space. Then the followings are valid: (i) πΊ β π is called β-open set if and only if every point of πΊ has a β-neighborhood contained in πΊ. Also πΊ β π is called β-closed set if and only if its complement is β-open. (ii) The β-interior πΊπ is the largest β-open set contained in πΊ and the β-closure πΊ is the smallest β-closed set contained in πΊ. Definition 12 (usual β-topology). Consider the set of βcomplex numbers with .. Proposition 8 (see [15]). Let π β₯ 1 and π§πβ , π‘πβ β Cβ for π β {0, 1, 2, 3, . . . , π}. Then (π½ β β π§πβ β π‘πβ β ) .. 2π½ .. (13) β .. .. Definition 10. Given a point π₯0 β π. Then, for a positive π½real number π, β π§πβ = π§0β β π§1β β π§2β β β β β β π§πβ β β β β β β 2 = (πΌ {(πΌβ1 (π1 )) + (π½β1 (π1 )) } , 0 ) = β π§β β . π = {π β Cβ | βπ₯ β π, βπ > 0 β π΅β (π₯0 ; π) β π} β (19) β for all π₯0 β C and π β Rπ½ . Then (C , π) is a topological space and is called β-usual topology on Cβ . Definition 13. (i) A topological β-vector (linear) space π is a β-vector space (see [17]) over the topological field that endowed with a topology such that β-vector addition and scalar multiplication are β-continuous functions. (ii) A topological β-vector space is called β-normable if the topology of the space can be induced by a β-norm. Definition 14. A sequence space π with a β-linear topology is called a βK-space provided each of the maps ππ : π β Cβ defined by ππ (π₯) = π₯π is β-continuous for all π β N. A βKspace is called a βFK-space provided π is a complete linear β-metric space (see [15]). An βFK-space whose topology is β-normable is called a βBK-space. Definition 15 (π-βnormed space). Let π be a real or complex .. .. β-linear space and let β β β π be a function from π to the set .. .. R+π½ and π > 0. Then the pair (π, β β β π ) is called a π-βnormed }) . .. .. space and β β β π is a π-βnorm for π, if the following axioms are satisfied for all elements π₯, π¦ β π and for all scalars π: Journal of Probability and Statistics .. .. 5 .. . .. (N1) β π₯ β π = 0 β π₯ = πβ (πβ = ( 0 , 0 )), .. .. .. .. ππ½ .. .. .. .. .. (N2) β π β π₯ β π = β π β modulus), .. .. .. .. .. .. .. × β π₯ β π ( β π β is complex .. (N3) β π₯ β π¦ β π β€ β π₯ β π + β π¦ β π . β Definition 16. (i) A β-linear map or β-linear operator π between real (or complex) β-linear spaces π, π is a function . . . . . . π : π β π such that π(π × π₯ + π × π¦) = π × ππ₯ + π × ππ¦ for β β β all π, π β RπΌ and similarly π(π βπ₯βπ βπ¦) = π βππ₯βπβ βππ¦ for all πβ , πβ β Cβ and π₯, π¦ β π. (ii) Let π and π be two β-normed linear spaces. A βlinear map π : π β π is β-bounded if there is a constant .. .. .. .. .. .. .. .. π β₯ 0 such that β ππ₯ β π β€ π × β π₯ β π for all π₯ β π. We denote the set of all β-linear maps π : π β π by L(π, π) and the set of all β-bounded linear maps by B(π, π). 3. Non-Newtonian Infinite Matrices Let π€β denote the set of all β-complex sequences π₯ = (π₯π )β π=0 . β , πβ , π0β for the sets of all β-bounded, βAs usual, we write ββ convergent, β-null sequences and βπβ β = {π§ = (π§πβ ) β β .. βπ :ββ π=1 provided the series on the right hand side converge. On the other hand the series on the right hand side of (22) converges if and only if β π§πβ β (πΌβ1 (πππ ) πΌβ1 (πππ ) β π½β1 (πΏππ ) π½β1 (πππ )) , π=0 (23) β β1 β < β} (20) β (πΌ (πππ ) π½ (πππ ) + π½ (πΏππ ) πΌ (πππ )) are convergent classically. However the series (22) may βdiverge for some, or all, values of π, π; the product π΄ β π΅ may not exist. β ) = (πππ , πΏππ ) be an infinite Let π1β , π2β β π€β , and π΄ = (πππ matrix of β-complex numbers. Then we say that π΄ defines a matrix mapping from π1β into π2β and denote it by writing π΄ : π1β β π2β , if for every sequence π§ = (π§πβ ) β π1β the sequence π΄ β π§ = {(π΄π§)π }, the π΄-transform of π§, exists and is in π2β . In this way, we transform the sequence π§ = (π§πβ ) = (ππ , ππ ) with ππ β RπΌ and ππ β Rπ½ , into the sequence {(π΄π§)π } by β {(π΄π§)π } = β βπππ β π§πβ π β π΄ β π΅ = (πππβ β πππβ ) = (πππ , πΏππ ) β (πππ , πππ ) .. = (πππ + πππ , πΏππ + πππ ) = (πΌ {πΌβ1 (πππ ) + πΌβ1 (πππ )} , π½ {π½β1 (πΏππ ) + π½β1 (πππ )}) , (21) πβ β π΄ = (πβ β πππβ ) .. = ( π , π ) β (πππ , πΏππ ) = (πΌ {ππππ β ππΏππ } , π½ {ππππ + ππΏππ }) , . .. (πβ = ( π , π ) β Cβ ) , where πππ , πππ β RπΌ and πΏππ , πππ β Rπ½ for all π, π β N. Also, the product (π΄ β π΅)ππ of π΄ = (πππβ ) and π΅ = (πππβ ) can be interpreted as β β β = β β πππ β πππ π=0 β = (πΌ { β (πΌβ1 (πππ ) πΌβ1 (πππ ) β π½β1 (πΏππ ) π½β1 (πππ ))} , (22) π=0 β π½ { β (πΌβ1 (πππ ) π½β1 (πππ ) + π½β1 (πΏππ ) πΌβ1 (πππ ))}) π=0 β1 .. .. π A non-Newtonian infinite matrix π΄ = (πππβ ) of β-complex numbers is defined by a function π΄ from the set N×N into Cβ . The addition (β) and scalar multiplication (β) of the infinite matrices π΄ = (πππβ ) = (πππ , πΏππ ) and π΅ = (πππβ ) = (πππ , πππ ) are defined by . β1 π=0 for 1 β€ π < β. . β1 = (πΌ { β (πΌβ1 (πππ ) πΌβ1 (ππ ) β π½β1 (πΏππ ) π½β1 (ππ ))} , π=0 (24) β π½ { β (πΌβ1 (πππ ) π½β1 (ππ ) + π½β1 (πΏππ ) πΌβ1 (ππ ))}) π=0 for all π, π β N. Thus, π΄ β (π1β : π2β ) if and only if the series on the right side of (24) β-converges for each π β N and every π§ β π1β , and we have π΄ β π§ = {(π΄π§)π }πβN β π2β for all π§ β π1β . A sequence π§ is said to be π΄-summable to πΎ if π΄βπ§ β-converges to πΎ β Cβ which is called π΄-β lim of π§. The CesaΜro transform of a sequence π§ = (π§πβ ) β π€β is given by πΆ1β β π§ = {(πΆ1β π§)π }πβN . Now, following Example 17 we may state the CesaΜro summability with respect to the nonNewtonian calculus which is analogous to the classical CesaΜro summable. β ) by Example 17. Define the matrix πΆ1β = (πππ β πππ (πΌ, π½) 1 1 β 1 { ( ) = (πΌ ( ),π½( )) , 0 β€ π β€ π, (25) { { { π+1 π+1 π+1 ={ { { { β π > π. {0 = (πΌ (0) , π½ (0)) , If we choose the generator functions as πΌ = exp and π½ = exp, then the infinite matrix can be written as follows: 6 Journal of Probability and Statistics (π, π) (1, 1) β β β β β β β β β (βπ, βπ) β β β β β β (βπ, βπ) (1, 1) ( 3 3 3 3 3 3 ( (βπ, βπ) βπ) βπ) (βπ, (βπ, β β β (1, 1) ( ( β ( πππ (exp, exp) = ( .. .. .. .. . . . d . ( ( ( π+1 π+1 βπ, π+1 βπ) ( π+1 βπ, π+1 βπ) β β β ( π+1 βπ, π+1 βπ) ( βπ, βπ) ( π+1 .. . ( .. . .. . The πΆ1β -transform of a sequence π₯ = (π₯πβ ) = (ππ , ππ ) is the sequence π¦ = (π¦πβ ) defined by π₯πβ . β π=1 π π π = (πΌ β .π β , π=1 π π β ..π :) π½ π=1 π (27) where (β is β-complex division), ππ β RπΌ , and ππ β Rπ½ for all π β N. Taking πΌ = exp and π½ = exp, we obtain πΆ1β -transform of π₯ = (π₯πβ ) = (ππ , ππ ) as follows: π¦πβ = (πΆ1β β π₯)π 1 π 1 π = (exp { β ln (ππ )} , exp { β ln (ππ )}) π π=1 π π=1 = ((π1 β β β ππ ) 1/π , (π1 β β β ππ ) ) β β β ) ) ) .. ) ). . ) ) ) β β β (26) d ) 4. Matrix Transformations Related to the Strong Cesàro β-Summability .. π 1 π 1 π = (πΌ { β πΌβ1 (ππ )} , π½ { β π½β1 (ππ )}) , π π=1 π π=1 1/π .. . β β β Let π and π(π) (π = 0, 1, . . .) be the sequences with ππ = 1β for all π β N and ππ(π) = 1β and ππ(π) = 0β for π =ΜΈ π. Also, if π is π¦πβ = (πΆ1β β π₯)π = β β π β β β β β β (28) ), a βBK-space and π β πβ then we write βπββ‘ = sup{ β ββ ππ β .. .. .. .. π₯π β : β π₯ β = 1}. Moreover, a βBK-space π β 0 is said to have βAK if every sequence π₯ = (π₯π )β π=1 β π has a unique β (π) representation π₯ = ββπ=1 π₯π β π . If π is a subset of π€β then ππ½ = {π β πβ : π β π₯ β ππ β for all π₯ β π} is called the π½-dual of π. Throughout the text we use the notation [πΆ1β ]π for strong CesaΜro β-summability of order 1 and index π. Maddox [19] introduced and studied the sets of sequences that are strongly summable and bounded with index π, (1 β€ π < β) by the CesaΜro method of order one. By taking into account the π π (πΌ, π½) of sequences that are sets π0 (πΌ, π½), ππ (πΌ, π½), and πβ strongly β-summable to zero, β-summable, and β-bounded of index π β₯ 1 are defined by (ππ , ππ β Rexp ) . .. ππ½ .. π { β π₯π β π π0 (πΌ, π½) = {π₯π = (ππ , ππ ) β πβ : π½ lim π½ β .. πββ π π=1 { .. } fl 0 } } (ππ β RπΌ , ππ β Rπ½ ) .. 2 2 π/2 1 π = {(ππ , ππ ) β πβ : lim π½ { β [(πΌβ1 {ππ }) + (π½β1 {ππ }) ] } = 0 } , πββ π π=1 .. ππ½ .. π { β π₯π β β β ππ (πΌ, π½) = {π₯π = (ππ , ππ ) β πβ : π½ lim π½ β .. πββ π π=1 { } .. fl 0 for some β β Cβ } } .. 2 2 π/2 1 π = {(ππ , ππ ) β πβ : lim π½ { β [(πΌβ1 {ππ } β πΌβ1 {β1 }) + (π½β1 {ππ } β π½β1 {β2 }) ] } = 0 , β = (β1 , β2 ) β Cβ } , πββ π π=1 .. .. ππ½ π { β π₯π β π πβ (πΌ, π½) = {π₯π = (ππ , ππ ) β πβ : sup π½ β .. π πβN π=1 { } .. .. 2 2 π/2 1 π : < β} = {(ππ , ππ ) β πβ : sup π½ { β [(πΌβ1 {ππ }) + (π½β1 {ππ }) ] } < β} . π π=0 πβN } (29) Journal of Probability and Statistics 7 .. .. ππ½ π { β π₯π β { { :, sup β { .. { π½ { π .. .. { πβN π=1 βπ₯ββ = { (1/π)π½ .. ππ½ .. { π { β π₯π β { { { sup ( , :) β .. { π½ π πβN π=1 { For instance, π (i) π0 (exp, ππ ) = {(ππ , ππ ) β πβ : limπββ {(1/ π) βππ=1 (ln2 (ππ ) + (ππ )2π )π/2 }1/π = 0}, (ππ β Rexp , ππ β Rπ , π β R+ , π β₯ 1); (ii) ππ (ππ , exp) = {(ππ , ππ ) β πβ : limπββ {(1/ π) βππ=1 [((ππ )π β (β1 )π )2 + ln2 (ππ /π2 )]π/2 } = 0}, (ππ , β1 β Rπ ; ππ , β2 β Rexp ). .. (32) (1/π)π½ .. ππ½ .. , . :) Proof. The proof is straightforward (see [20]). π First we give the π½-duals of the spaces π0 (πΌ, π½), ππ (πΌ, π½), π (πΌ, π½). We prefer the notation β] and max] for the and πβ sum and maximum taken over all indices π with 2] β€ π β€ 2]+1 β 1 and put Proof. The proof is a routine verification and hence omitted. π π Corollary 19. The sets π0 (πΌ, π½), ππ (πΌ, π½), and πβ (πΌ, π½) (πΌ,π½) are Banach spaces with the induced metric ππ from the (πΌ,π½) Mπ .. corresponding norm β π₯ β β defined by .. = {π§ β πβ : βπ§βMπ < β} , (33) where β π :) β π₯π β = sup (π½ β .. π πβN π=1 β β π₯π β π¦π β { { { :, 0 < π < 1, sup π½ β .. { { π (30) { { πβN π=1 fl { (1/π)π½ .. ππ½ .. { { { π β π₯π β π¦π β } { { {sup {π½ β , 1 β€ π < β. :} .. { π πβN { { π=1 } βπ§βM(πΌ,π½) π βπ₯ββ ππ (πΌ,π½) .. ππ½ (1/π)π½ .. ππ½ βπ₯ β = sup (π½ β π]π½ 2 ]βN ] π βπ₯βπβ (πΌ,π½) ππ(πΌ,π½) (π₯, π¦) .. 1 β€ π < β. π π .. (31) Proposition 20. Let 1 β€ π < β. The sets π0 (πΌ, π½), ππ (πΌ, π½), π (πΌ, π½) are βBK-spaces with the (equivalent) β-norms and πβ π (πΌ, π½) are Theorem 18. The sets π0 (πΌ, π½), ππ (πΌ, π½), and πβ (πΌ,π½) β complete β-metric spaces over the field C with the metric ππ defined by π 0 < π < 1, .. .. .. ]π½ .. { { β 2 × max β π§π β , { π½ { ] { { ]=0 { ={ { (1/π)π½ β { .. ππ½ .. { .. (]/π)π½ .. { { × ( β π§ β ) , β β {π½ 2 π π½ ] { ]=0 π = 1, (πΌ,π½) (1 < π < β; π = π ), (π β 1) βπ§ β Mπ . (34) In particular, we have β βπ§βM(exp,exp) π .. for all π§π = (ππ , ππ ) β πβ where ππ , ππ β Rexp = (0, β). β Now, with regard to notation, for any matrix π΄ = (πππ ) we write, for 1/π + 1/π = 1, π β₯ 1, .. ππ½ .. β π΄π] (π) = (π½ β β πππ β ) (1/π)π½ (36) ] and the case π = 1 of (36) is interpreted as .. .. β π΄1] (π) = max β πππ β. ] .. β .. .. 2] { exp { β 2] ln (max β π§π β )} = β (max β π§π β ) , π = 1, { { ] ] { { ]=0 ]=0 ={ 1/π β { .. π .. { { {exp { β 2]/π (β (ln β π§π β ) ) } , 1 < π < β, ] { ]=0 (37) (35) Remark 21. Let π be a β-normed space and let π be a β-linear operator on the π-βnormed space π into π. Then it is easy to see that π is β-continuous on π if and only if there is a positive .. .. .. .. .. .. (1/π)π½ on π. constant π β Rπ½ such that β ππ₯ β π β€ π × β π₯ β π The β-norm on the left is the norm in π and that on the right is π-βnorm in π. It is also seen that Banach-Steinhaus theorem in the non-Newtonian sense holds in a π-βnormed space defined in Definition 15. Also one can immediately conclude that [πΆ1β ]π is βcomplete in the metric generated by the β-norm. For simplicity we denote [πΆ1β ]π by Ξ©, so that, in the case π β₯ 1, Ξ© 8 Journal of Probability and Statistics is a Banach space and, in the case 0 < π < 1, Ξ© is a complete π-βnormed space. The dual space of Ξ©, that is, the space of continuous β-linear functionals on Ξ©, will be denoted by Ξ©β . To prove uniformly β-convergent, by using the conjugate numbers π and π for 0 < π < 1, then, for any positive integer π0 and for any π β₯ 2π0 , we obtain β .. Corollary 22 (cf. [19] (Banach-Steinhaus)). If (ππ ) is a sequence of continuous β-linear operators on a πβnormed space π into a β-normed space π such that .. .. .. π½ lim supπ β ππ π₯ β π < β on a second category set in π, then .. supπ βππ β < β. It is important to remark that βππ β denotes the .. .. .. .. π=π The next theorem characterizes all infinite matrices π΄ which map the space [πΆ1β ]π into the space πβ of convergent sequences of β-complex numbers. Theorem 23. (π΄π§)π is defined for each π and the sequence {(π΄π§)π } is β-convergent, whenever π§ β Ξ©, if and only if, (a) for 0 < π < 1, .. (]/π)π½ .. β€ π½ β π΄1] ]=π0 (ii) π = supπ {π½ ββ ]=0 2 × π΄1] (π)} < β; (i) as in (a) above, .. (]/π)π½ .. β β (iii) π = β π½ β π=1 β β πππ β where π§π .. .. .. β .. (]/π)π½ .. × max] β ππ β β€ π, π½ β]=0 2 holds .. .. β .. .. .. (43) ] = 0 , (π β β). for each π and each ] β₯ 0. They are β-linear and β-continuous since .. .. .. .. .. (]/π)π½ .. .. β β β βπππ β π§π β β€ π΄1] (π) × 2 .. 1/π × βπ§βπ . ] .. .. .. .. .. .. (1/π)π½ .. .. .. .. ππ½ (38) (1/π)π½ .. (]/π)π½ .. β€ π½ β π΄1] (π) × 2 .. .. (β1/π)π½ × sgn π§π,π] , π§π = 0β (π =ΜΈ π] ), for 0 β€ ] β€ π , .. .. .. .. where π] is such that β π§π,π] β = max] β ππ,π β . By (45) we .. .. (]/π)π½ .. .. 1/π × βπ§βπ .. .. β€π× .. .. 1/π .. βπ§βπ < β. β ]=0 Again for 0 < π < 1 we will show that the conditions (i) and (ii) imply (iii). In fact we will prove that (ii) which implies .. .. β ββ π=0 β πππ β is uniformly β-convergent (see Definition 7) and this together with (i) gives lim π π§π] = 2 have π½βπ ]=0 π΄1] (π) × 2 ] β (45) .. (]/π)π½ .. ] .. , where βπ΄ π β = supπ β (π΄π§)π β × β π§ β π . Taking any β integer π > 0 and define π§ β Ξ© by π§π = 0 for π β₯ 2π +1 and .. .. (44) β From Corollary 22, it follows that lim] ββ] πππ β π§π = (π΄π§)π is β in Ξ© , whence .. .. imply (42) β (π΄π§)π β β€ β π΄ π β × β π§ β π β β€ π½ β (π½ β β πππ β π§π β ) ]=0 (i)-(ii) β β π§π σ³¨β β β ππ β π§π β πππ β π§π β β and β β β βπππ β π§π β β Ξ©β , β β π§π β = π½ β π½ β β πππ ]=0 β, (41) and we deduce that β π§ is absolutely β-convergent and the last sum in (41) π β π β ..π goes to 0 as π β β. From (39), .. β . β β β ππ )] β β β (πππ β ππ ) (π§π β β) β ππ β π§π β [β β β β (πππ .. Proof. The proofs of necessity condition of (i) and (iii) and the sufficiency of the conditions are routine verification and hence omitted. Firstly we prove the sufficiency when 0 < π < 1, leaving the necessities (ii) and (ii)σΈ to the next. Now, consider that the condition (ii) holds. Then the series defining (π΄π§)π is absolutely β-convergent (see Definition 7) for each π β N. By using the known inequality we have β .. β€π× 2 (40) β β π§π β πππ × π΄π] (π) < β, β (βββ π=0 πππ , π) (π) × 2 .. .. (π0 /π)π½ for every π§ β πβ . Also, the sufficiency for the case π β₯ 1 can be obtained in a similar way. Conversely suppose that (π΄π§)π exists for each π β₯ 1 whenever π₯ β Ξ©. Thus, the functionals (b) for π β₯ 1, (ii)σΈ π = π½ ββ ]=0 2 .. .. ]π½ .. Thus, β .. ] β .. .. β (i) πβ (πππ , ππ ) = 0 (π β β, π fixed), .. .. ]=π0 .. (β1/π)π½ norm of ππ , that is, βππ β = supπ β ππ π₯ β π × β π₯ β π , the supremum being taken over all non-π½-zero elements of π. β .. .. β β β β€ π½ β π½ β β πππ β β β πππ π½ β β πππ β = β β ππ . (39) β€ βπ΄ π β for each π and implies σ΅© σ΅© .. β€ σ΅©σ΅©σ΅©π΄ π σ΅©σ΅©σ΅© < β. .. .. (]/π)π½ .. β π΄1] (π) × 2 π½ ]=0 (46) In fact the series (π΄π§)π was absolutely β-convergent which gives β .. .. (]/π)π½ σ΅©σ΅© σ΅©σ΅© .. 1 . σ΅©σ΅©π΄ π σ΅©σ΅© β€ π½ β π΄ ] (π) × 2 ]=0 (47) Journal of Probability and Statistics 9 π From (46) and (47), it can easily be seen that β .. .. (]/π)π½ σ΅©σ΅© σ΅©σ΅© 1 . σ΅©σ΅©π΄ π σ΅©σ΅© = π½ β π΄ ] (π) × 2 (48) ]=0 This leads us together with Corollary 22 to the fact that β .. (]/π)π½ .. 1 .. σ΅© σ΅© sup σ΅©σ΅©σ΅©π΄ π σ΅©σ΅©σ΅© = sup {π½ β 2 × π΄ ] (π)} < β. π π (49) ]=0 Similarly, one can prove that (ii)σΈ is necessary condition. This completes the proof. Now, as an immediate consequence of Theorem 23, the π following corollary shows the π½-duals for π0 (πΌ, π½), ππ (πΌ, π½), π and πβ (πΌ, π½). π Corollary 24. The π½-duals of the spaces π0 (πΌ, π½), ππ (πΌ, π½), (πΌ,π½) π and πβ (πΌ, π½) are Mπ . Remark 25. The symbol βπ½β used for π½-dual has different meaning from that of π½ generator used in the text. We may give with quoting the following proposition and lemma without proofs (see [21, 22]) which are needed in the proof of next theorem. Proposition 26. Let π be a βBK-space. Then we have π΄ β β β ) if and only π΄ π β ππ½ for all π β N where π΄ π = (πππ ) (π : ββ for the sequence in the πth row of π΄ for all π β N. β ) be an innite matrix. If Lemma 27. Let π΄ = (πππ .. .. π½ βπ΄ π βM(πΌ,π½) < β and limπββ βπ΄ π βM(πΌ,π½) = 0 , then βπ΄ π βM(πΌ,π½) π π π uniformly β-converges in π β N. π β π β β (i) π΄ = (πππ ) β (πβ (πΌ, π½) : ββ ) = (π0 (πΌ, π½) : ββ ) = π β (π (πΌ, π½) : ββ ) if and only if σ΅© σ΅© sup σ΅©σ΅©σ΅©π΄ π σ΅©σ΅©σ΅©M(πΌ,π½) < β. π .. πβN (50) β π ) β (πβ (πΌ, π½) : π0β ) if and only if (ii) π΄ = (πππ .. σ΅© σ΅© lim σ΅©σ΅©π΄ σ΅©σ΅© (πΌ,π½) = 0 . πββ σ΅© π σ΅©Mπ (51) π β ) β (π0 (πΌ, π½) : π0β ) if and only if (50) holds (iii) π΄ = (πππ and β lim πβ πββ ππ = 0β (52) for all π β N. β (πππ ) (iv) π΄ = hold and π β (π (πΌ, π½) : β π0β ) if and only if (50), (52) β β lim β β πππ = 0β . πββ π=1 5. Concluding Remarks Non-Newtonian calculus is a methodology that allows one to have a different look at problems which can be investigated via calculus. It should be clear that the non-Newtonian calculus is a self-contained system independent of any other system of calculus. Therefore the reader may be surprised to learn that there is a uniform relationship between the corresponding operators of this calculus and the classical calculus. In this paper we have introduced the sequence spaces π π (πΌ, π½) as a generalization of the π0 (πΌ, π½), ππ (πΌ, π½), and πβ π π π spaces π0 , π , and πβ of Maddox [19]. Our main purpose is π to determine the π½-duals of the new spaces π0 (πΌ, π½), ππ (πΌ, π½), π and πβ (πΌ, π½) and is to characterize the classes of matrix transformations from these spaces to any one of the spaces β , πβ , and π0β . As a future work we will try to obtain the ββ characterizations of the classes of infinite matrices from the π π (πΌ, π½) to a sequence space spaces π0 (πΌ, π½), ππ (πΌ, π½), and πβ β , π over the non-Newtonian complex field different from ββ β β π , and π0 . Competing Interests Theorem 28. The following statements hold: π½ β ) follows Proof. (i) Condition (50) for π΄ β (π0 (πΌ, π½) : ββ from Proposition 26 and Corollary 24. Then the other parts π π (πΌ, π½) by follows from the fact that π0 (πΌ, π½) β ππ (πΌ, π½) β πβ Proposition 20. (ii) This condition is proved in the same way as in Theorem 23 with ππ = 0β for all π β N. π (iii) Since π0 (πΌ, π½) is a βBK-space with βAK by Propoβ β β the conditions sition 20 and π , π0 are closed subset of ββ π β follow from the characterization of (π0 (πΌ, π½) : ββ ). (iv) The conditions follow from those in (iii). (53) The author declares that there are no competing interests. References [1] M. Zeltser, M. Mursaleen, and S. A. Mohiuddine, βOn almost conservative matrix methods for double sequence spaces,β Publicationes Mathematicae, vol. 75, no. 3-4, pp. 387β399, 2009. [2] U. Kadak and P. 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