z-logo
open-access-imgOpen Access
A Characterization for Fourier Hyperfunctions
Author(s) -
Jaeyoung Chung,
SoonYeong Chung,
Dohan Kim
Publication year - 1994
Publication title -
publications of the research institute for mathematical sciences
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.786
H-Index - 39
eISSN - 1663-4926
pISSN - 0034-5318
DOI - 10.2977/prims/1195166129
Subject(s) - mathematics , characterization (materials science) , fourier transform , mathematical analysis , materials science , nanotechnology
The space of test functions for Fourier hyperfunctions is characterized by two conditions sup| 0. Combining this result and the new characterization of Schwartz space in [1] we can easily compare two important spaces J and 3 which are both invariant under Fourier transformations. § 0. Introduction The purpose of this paper is to give new characterization of the space £F of test functions for the Fourier hyperfunctions. In [6], K. W. Kim, S. Y. Chung and D. Kim introduce the real version of the space EF of test functions for the Fourier hyperfunctions as follows, *- 0\. They also show the equivalence of the above definition and Sato-Kawai's original definition in complex form. Also, in [1] J. Chung, S. Y. Chung and D. Kim give new characterization of the Schwartz space S, i.e., show that for O) |exp&|%| 0. Observing the above growth conditions we can easily see that the space £F which is invariant under the Fourier transformation is much smaller than Communicated by T. Kawai, April 5, 1993. Revised May 20, 1993. 1991 Mathematics Subject Classification: 46F12, 46F15. * Department of Mathematics, Kunsan National University, Kunsan 573-360, Korea. ** Department of Mathematics, Duksung Women's University, Seoul 132-714, Korea. Department of Mathematics, Seoul National University, Seoul 151-742, Korea. Partially supported by the Ministry of Education and GARC. 204 JAEYOUNG CHUNG, SOON-YEONG CHUNG AND DOHAN KIM Schwartz space S. Since an element in the strong dual £F' of the space 3 is called a Fourier hyperfunction, the space 9"' of Fourier hyperfunctions which is also invariant under the Fourier transformation is much bigger than the space S of tempered distributions. Section 1 is devoted to providing the necessary definitions and preliminaries. We prove the main theorem in Section 2. § 1. Preliminaries We use the multi-index notations; for x = (xl} , xn\ f = (&, , fn)e/2 n and a multi-index a=(a1} az, , aJejV?, 8 =d^ dfi, \a =«H ----\-an with dj=d/dxjf and NQ the set of non-negative integers. For f^L(R] the Fourier transform / is the bounded continuous function in R defined by (1.1) Definition 1.1. We denote by (;c)i

The content you want is available to Zendy users.

Already have an account? Click here to sign in.
Having issues? You can contact us here
Accelerating Research

Address

John Eccles House
Robert Robinson Avenue,
Oxford Science Park, Oxford
OX4 4GP, United Kingdom