<p>We perform an asymptotic evaluation of the Hankel transform, <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11139_2025_1025_Article_IEq1.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="129" /> </InlineMediaObject> <EquationSource Format="TEX">\(\int _0^{\infty }J_{\nu }(\lambda x) f(x)\textrm{d}x\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mo>∫</mo> <mn>0</mn> <mi>∞</mi> </msubsup> <msub> <mi>J</mi> <mi>ν</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>λ</mi> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mtext>d</mtext> <mi>x</mi> </mrow> </math></EquationSource> </InlineEquation>, for arbitrarily large <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11139_2025_1025_Article_IEq2.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="TEX">\(\lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>λ</mi> </math></EquationSource> </InlineEquation> of an entire exponential type function, <i>f</i>(<i>x</i>), of type <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11139_2025_1025_Article_IEq3.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="11" /> </InlineMediaObject> <EquationSource Format="TEX">\(\tau \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>τ</mi> </math></EquationSource> </InlineEquation> by shifting the contour of integration in the complex plane. Under the situation that <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11139_2025_1025_Article_IEq4.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="82" /> </InlineMediaObject> <EquationSource Format="TEX">\(J_{\nu }(\lambda x)f(x)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>J</mi> <mi>ν</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>λ</mi> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> has an odd parity with respect to <i>x</i> and the condition that the asymptotic parameter <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11139_2025_1025_Article_IEq5.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="TEX">\(\lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>λ</mi> </math></EquationSource> </InlineEquation> is greater than the type <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11139_2025_1025_Article_IEq6.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="11" /> </InlineMediaObject> <EquationSource Format="TEX">\(\tau \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>τ</mi> </math></EquationSource> </InlineEquation>, we obtain an exactly terminating Poincaré expansion without any trailing subdominant exponential terms. That is, the Hankel transform evaluates exactly into a polynomial in inverse <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11139_2025_1025_Article_IEq7.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="TEX">\(\lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>λ</mi> </math></EquationSource> </InlineEquation> as <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11139_2025_1025_Article_IEq8.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="TEX">\(\lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>λ</mi> </math></EquationSource> </InlineEquation> approaches infinity.</p>

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Terminating Poincaré asymptotic expansion of the Hankel transform of entire exponential type functions

  • Nathalie Liezel R. Rojas,
  • Eric A. Galapon

摘要

We perform an asymptotic evaluation of the Hankel transform, \(\int _0^{\infty }J_{\nu }(\lambda x) f(x)\textrm{d}x\) 0 J ν ( λ x ) f ( x ) d x , for arbitrarily large \(\lambda \) λ of an entire exponential type function, f(x), of type \(\tau \) τ by shifting the contour of integration in the complex plane. Under the situation that \(J_{\nu }(\lambda x)f(x)\) J ν ( λ x ) f ( x ) has an odd parity with respect to x and the condition that the asymptotic parameter \(\lambda \) λ is greater than the type \(\tau \) τ , we obtain an exactly terminating Poincaré expansion without any trailing subdominant exponential terms. That is, the Hankel transform evaluates exactly into a polynomial in inverse \(\lambda \) λ as \(\lambda \) λ approaches infinity.