Abstract

The Hankel transformation was extended by Zemanian to certain generalized functions of slow growth through a generalization of Parsevalā€™s equation as ( ( 1 ) ) āŸØ h Ī¼ f , Ļ† āŸ© = āŸØ f , h Ī¼ Ļ† āŸ© \begin{equation}\tag {$(1)$} \langle {h_\mu }f,\varphi \rangle = \langle f,{h_\mu }\varphi \rangle \end{equation} where Ļ† , h Ī¼ Ļ† āˆˆ H Ī¼ , f āˆˆ H Ī¼ ā€² \varphi , {h_\mu }\varphi \in {H_\mu }, f \in {Hā€™_\mu } . Later, Koh and Zemanian defined the generalized complex Hankel transformation on J Ī¼ = ā‹ƒ Ī½ = 1 āˆž J a Ī½ , Ī¼ {J_\mu } = {\bigcup }_{\nu = 1}^\infty \,{J_{{a_\nu },\mu }} , where J a Ī½ , Ī¼ {J_{{a_\nu },\mu }} is the testing function space which contains the kernel function, x y J Ī¼ ( x y ) \sqrt {xy} {J_\mu }(xy) . A transformation was defined directly as the application of a generalized function to the kernel function, i.e., for f āˆˆ J Ī¼ ā€² f \in {Jā€™_\mu } , ( ( 2 ) ) ( h Ī¼ f ) ( y ) = āŸØ f ( x ) , x y J Ī¼ ( x y ) āŸ© . \begin{equation}\tag {$(2)$} ({h_\mu }f)(y) = \langle f(x),\sqrt {xy} {J_\mu }(xy)\rangle .\end{equation} In this paper, we extend definition (2) to a larger space of generalized functions. We first introduce the test function space M a , Ī¼ {M_{a,\mu }} which contains the kernel function and show that H Ī¼ āŠ‚ M a , Ī¼ āŠ‚ J a , Ī¼ {H_\mu } \subset {M_{a,\mu }} \subset {J_{a,\mu }} . We then form the countable union space M Ī¼ = ā‹ƒ Ī½ = 1 āˆž M a Ī½ , Ī¼ {M_\mu } = {\bigcup }_{\nu = 1}^\infty \,{M_{{a_\nu },\mu }} whose dual M Ī¼ ā€² {Mā€™_\mu } has J Ī¼ ā€² {Jā€™_\mu } as a subspace. Our main result is an inversion theorem stated as follows. Let F ( y ) = ( h Ī¼ f ) ( y ) = āŸØ f ( x ) , x y J Ī¼ ( x y ) āŸ© , f āˆˆ M Ī¼ ā€² F(y) = ({h_\mu }f)(y) = \langle f(x),\sqrt {xy} {J_\mu }(xy)\rangle ,f \in {Mā€™_\mu } , where y is restricted to the positive real axis. Let Ī¼ ā‰„ āˆ’ 1 2 \mu \geq - \frac {1}{2} . Then, in the sense of convergence in H Ī¼ ā€² {Hā€™_\mu } , \[ f ( x ) = lim r ā†’ āˆž āˆ« 0 r F ( y ) x y J Ī¼ ( x y ) d y . f(x) = \lim \limits _{r \to \infty } \int _0^r {F(y)} \sqrt {xy} {J_\mu }(xy)dy. \] This convergence gives a stronger result than the one obtained by Koh and Zemanian (1968). Secondly, we prove that every generalized function belonging to M a , Ī¼ ā€² {Mā€™_{a,\mu }} can be represented by a finite sum of derivatives of measurable functions. This proof is analogous to the method employed in structure theorems for Schwartz distributions (Edwards, 1965), and similar to one by Koh (1970).

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