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Weierstrass Transform on Howell's Space-A New Theory

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Weierstrass Transform on Howell's Space-A New Theory IOSR Journal of Mathematics (IOSR-JM) e-ISSN: 2278-5728, p-ISSN: 2319-765X. Volume 16, Issue 6 Ser. IV (Nov. – Dec. 2020), PP 57-62 www.iosrjournals.org Weierstrass Transform on Howell’s Space-A New Theory 1 2* 3 V. N. Mahalle , S.S. Mathurkar , R. D. Taywade 1(Associate Professor, Dept. of Mathematics, Bar. R.D.I.K.N.K.D. College, Badnera Railway (M.S), India.) 2*(Assistant Professor, Dept. of Mathematics, Govt. College of Engineering, Amravati, (M.S), India.) 3(Associate Professor, Dept. of Mathematics, Prof. Ram Meghe Institute of Technology & Research, Badnera, Amravati, (M.S), India.) Abstract: In this paper we have explained a new theory of Weierstrass transform defined on Howell’s space. The definition of the Weierstrass transform on this space of test functions is discussed. Some Fundamental theorems are proved and some results are developed. Weierstrass transform defined on Howell’s space is linear, continuous and one-one mapping from G to G c is also discussed. Key Word: Weierstrass transform, Howell’s Space, Fundamental theorem. --------------------------------------------------------------------------------------------------------------------------------------- Date of Submission: 10-12-2020 Date of Acceptance: 25-12-2020 --------------------------------------------------------------------------------------------------------------------------------------- I. Introduction A new theory of Fourier analysis developed by Howell, presented in an elegant series of papers [2-6] n supporting the Fourier transformation of the functions on R . This theory is similar to the theory for tempered distributions and to some extent, can be viewed as an extension of the Fourier theory. Bhosale [1] had extended Fractional Fourier transform on Howell’s space. Mahalle et. al. [7, 8] described a new theory of Mellin and Laplace transform defined on Howell’s space. Motivated by the above work, we are extending this theory to Weierstrass transform. In this paper, we have introduced the concept of Weierstrass transform defined on Howell’s space. In section II new notation and basic spaces are discussed. We have proved one lemma and and fundamental theorem described in section III. Definition of Weierstrass transform on Howell’s space is given in Section IV. Some results are proved in section V. The Weierstrass transform defined on this space is linear, continuous and one-one, is proved in the form of theorems in section VI. Lastly conclusion is given. II. Notations and Conventions The notations, conventions and the terminologies in this work follow those of [2] and Zemanian [9]. Throughout this paper n will denote some arbitrary fixed positive integer and will denote the Lebesgue n measure on R . Unless otherwise indicated, all functions are to be assumed to have domain in C n and the 1 range in C . The notations y y 1 , y 2 ,....., y n and i will be considered interchangeable and all denote the n -dimensional complex variable with real part 1 , 2 ,...., n and imaginary part 1 , 2 ,....., n . 2.1 Here we list some notation form Howell [2], which will be used prominently in this work. n n (1) The translation: Let f : C C . For each C , f will denote the translation of f by , given by f | y f y . (2) Scaling operator: For each C , f will denote the function f with variable scaled by , that is f | f y y n (3) Exponential function: Let C . Where convenient, e will denote the function given by y e y e DOI: 10.9790/5728-1606045762 www.iosrjournals.org 57 | Page Weierstrass Transform on Howell’s Space-A New Theory (4) Normal Gaussian: Let 0 . Where convenient will denote the function given by 2 n y 2 y exp 2 n (5) Rho seminorm: The symbol will be reserved for the seminorm on C n given by y Re y k k 1 n n (6) Strips in C : For each 0 , B will denote the subset of C given by, n B y y 1 , y 2 ,....., y n C : | Im y k , k 1,2 ,....., n n Note that B 0 R and that if , then B B . 2.2 Basic Spaces G and G c : Two spaces of functions will be of especial importance. They will be denoted by G and G c and are defined below: 2.2.1 Definition G : A function : C n C , is an element of G if and only if both of the following holds: (1) is an analytic function of each complex variable. y (2) For every 0 , Sup e y : y B c n 2.2.2 Definition G : A function f : C C , is an element of G c if and only if both of the following holds: (1) f is an analytic function of each complex variable ( y ) (2) For every 0 there is a Corresponding 0 such that Sup {e f y : y B } G with suitable topology, will serve as the space of test functions. The following facts will be of importance and should all be obvious from the above definitions (1) G and G c both are linear spaces closed under multiplication. (2) G G c n (3) G contains all functions of the form , where 0 and C n n 1 n (4) If G and , C then e i is also in G and its restriction to R is in L R (5) G c contains all polynomial and exponential functions on C n n c (6) Any exponential function e with C is an element of G . The topology on G is defined by the set of norms . : 0, where y Sup e y : y B . Any function , which is analytic in each variable is clearly in G if and only if is finite for every 0 . It is also obvious that, if , then . c Similarly the topology on G is defined by the set of norms . : 0 where y Sup e y : y B , for every 0 , there is a corresponding 0 . c G with suitable topology will serve as the space of test functions. It is also obvious that, if , . A slightly more general relation is expressed in the following lemma. DOI: 10.9790/5728-1606045762 www.iosrjournals.org 58 | Page Weierstrass Transform on Howell’s Space-A New Theory 2.3 Lemma: Let 0 , k 0 and G .Then for any y B and C with , y k y y e e k Proof: Let y be any arbitrarily fixed elements of B and C with . Then k y Sup e y : y B k k y k y Sup e e y : y B k k y y e y e k Therefore, y k y y e e . k III. Fundamental Theorem C Let G and f G then mapping f is continuous linear mapping from G toG . Proof: Let and f are fixed elements of G and G c respectively. The analyticity of f is obvious and it c suffices to produce a suitable bound for f , where is arbitrary. Since f G , therefore for all 0 , there exists k 0 such that, k y e f y N (Say) (3.1) Now, to show that f G . y f Sup e f y y : y B , n where B denote the subset of C given in section II. But G then by lemma 2.3 with y k y y e e k Now, y k y e y f y e f y k (3.2) From equation (3.1), we get y e y f y N k Thus, for any G , f N k From this it follows that f is an element of G . Therefore the mapping f is continuous and linear from G to G . IV. Definition: Weierstrass transform on G For each f in G , W f be the function on C n given by, 2 x y 1 W f x f y e 4 d , y n 4 R where is explained in section II. This transform is well defined on G , since G c contains all polynomial and exponential functions on C n that 2 2 x y x y c is e 4 G . Hence for f y G , f y e 4 G by fundamental theorem. Now by property (4) 2 x y n 1 n p.no.344 of [2], restriction of f y e 4 G to R belongs to L R . Hence right hand side exists. DOI: 10.9790/5728-1606045762 www.iosrjournals.org 59 | Page Weierstrass Transform on Howell’s Space-A New Theory V. Elementary Weierstrass Analysis on G Here we have proved some results which are all analogous to well known results in the classical theory of Weierestrass transform for smooth integrable function on R n . 5.1 Result: (Scaling and Weierstrass transform on G): Let be any non zero real number and let f be any element of G . Then n W f x 1 W f x n n 5.2 Result: Let f G . Then for any and in C , W e f x 1 W e 1 f x 5.3 Result: (Differentiation and Weiertrass transform on G ): If f G , then W f is an analytic function of each variables and for k 1,2,3,..., n 1 i W k i k y k f i k 2 i i W k i k y k f i k 2 d x y x W f ( x ) dx 2 n 1 n 5.4 Result: If f , g G , then the restriction to R of the products gW f and f W g are in L R and g W f d f W g d n n R R 5.5 Result: (Transform of Normal Gaussian): 2 n y 1 4 The Weierstrass transform of Normal Gaussian is W y x W e x , 2 1 2 2 1 2 where .
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