<p>This paper investigates a broad class of non-Gaussian measures, <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\( \mu _\Psi \)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>μ</mi> <mi mathvariant="normal">Ψ</mi> </msub> </math></EquationSource> </InlineEquation>, associated with a family of generalized Wright functions, <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(_m\Psi _q\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mmultiscripts> <mrow /> <mi>m</mi> <mrow /> </mmultiscripts> <msub> <mi mathvariant="normal">Ψ</mi> <mi>q</mi> </msub> </mrow> </math></EquationSource> </InlineEquation>. First, we study these measures in Euclidean spaces <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\mathbb {R}^d\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>d</mi> </msup> </math></EquationSource> </InlineEquation>, then define them in an abstract nuclear triple <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\mathcal {N}\subset \mathcal {H}\subset \mathcal {N}'\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="script">N</mi> <mo>⊂</mo> <mi mathvariant="script">H</mi> <mo>⊂</mo> <msup> <mrow> <mi mathvariant="script">N</mi> </mrow> <mo>′</mo> </msup> </mrow> </math></EquationSource> </InlineEquation>. We study analyticity, invariance properties, and ergodicity under a particular group of automorphisms. Then we show the existence of an Appell system which allows the extension of the non-Gaussian Hilbert space <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(L^2(\mu _\Psi )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mn>2</mn> </msup> <mrow> <mo stretchy="false">(</mo> <msub> <mi>μ</mi> <mi mathvariant="normal">Ψ</mi> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> to the nuclear triple consisting of test functions and distributions spaces, <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\((\mathcal {N})^{1}\subset L^2(\mu _\Psi )\subset (\mathcal {N})_{\mu _\Psi }^{-1}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="script">N</mi> <mo stretchy="false">)</mo> </mrow> <mn>1</mn> </msup> <mo>⊂</mo> <msup> <mi>L</mi> <mn>2</mn> </msup> <mrow> <mo stretchy="false">(</mo> <msub> <mi>μ</mi> <mi mathvariant="normal">Ψ</mi> </msub> <mo stretchy="false">)</mo> </mrow> <mo>⊂</mo> <msubsup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="script">N</mi> <mo stretchy="false">)</mo> </mrow> <mrow> <msub> <mi>μ</mi> <mi mathvariant="normal">Ψ</mi> </msub> </mrow> <mrow> <mo>-</mo> <mn>1</mn> </mrow> </msubsup> </mrow> </math></EquationSource> </InlineEquation>. Furthermore, thanks to the definition of two transformations, <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(S_{\mu _{\Psi }}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>S</mi> <msub> <mi>μ</mi> <mi mathvariant="normal">Ψ</mi> </msub> </msub> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(T_{\mu _{\Psi }}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>T</mi> <msub> <mi>μ</mi> <mi mathvariant="normal">Ψ</mi> </msub> </msub> </math></EquationSource> </InlineEquation>, we study Donsker’s delta as an element within <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\((\mathcal {N})_{\mu _\Psi }^{-1}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="script">N</mi> <mo stretchy="false">)</mo> </mrow> <mrow> <msub> <mi>μ</mi> <mi mathvariant="normal">Ψ</mi> </msub> </mrow> <mrow> <mo>-</mo> <mn>1</mn> </mrow> </msubsup> </math></EquationSource> </InlineEquation> applying the integral equations fulfilled by <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(_m\Psi _q\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mmultiscripts> <mrow /> <mi>m</mi> <mrow /> </mmultiscripts> <msub> <mi mathvariant="normal">Ψ</mi> <mi>q</mi> </msub> </mrow> </math></EquationSource> </InlineEquation>.</p>

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Generalized Wright Analysis in Infinite Dimensions

  • Luisa Beghin,
  • Lorenzo Cristofaro,
  • José L. da Silva

摘要

This paper investigates a broad class of non-Gaussian measures, \( \mu _\Psi \) μ Ψ , associated with a family of generalized Wright functions, \(_m\Psi _q\) m Ψ q . First, we study these measures in Euclidean spaces \(\mathbb {R}^d\) R d , then define them in an abstract nuclear triple \(\mathcal {N}\subset \mathcal {H}\subset \mathcal {N}'\) N H N . We study analyticity, invariance properties, and ergodicity under a particular group of automorphisms. Then we show the existence of an Appell system which allows the extension of the non-Gaussian Hilbert space \(L^2(\mu _\Psi )\) L 2 ( μ Ψ ) to the nuclear triple consisting of test functions and distributions spaces, \((\mathcal {N})^{1}\subset L^2(\mu _\Psi )\subset (\mathcal {N})_{\mu _\Psi }^{-1}\) ( N ) 1 L 2 ( μ Ψ ) ( N ) μ Ψ - 1 . Furthermore, thanks to the definition of two transformations, \(S_{\mu _{\Psi }}\) S μ Ψ and \(T_{\mu _{\Psi }}\) T μ Ψ , we study Donsker’s delta as an element within \((\mathcal {N})_{\mu _\Psi }^{-1}\) ( N ) μ Ψ - 1 applying the integral equations fulfilled by \(_m\Psi _q\) m Ψ q .