<p>The aim of this paper is to establish a generalization of uncertainty principles for the <i>q</i>-Bessel Fourier transform, <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_976_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="30" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {F}_{q, \nu }\)</EquationSource> </InlineEquation> introduced earlier in Dhaouadi (Bull Math Anal Appl 5:42–60, 2013) and Dhaouadi (J Inequal Pure Appl Math 7:171, 2006). More precisely, we prove an <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_976_Article_IEq2.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="39" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {L}_{q,p,\nu }\)</EquationSource> </InlineEquation>-local uncertainty principle for <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_976_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="30" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {F}_{q, \nu }\)</EquationSource> </InlineEquation>, and we derive an <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_976_Article_IEq2.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="39" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {L}_{q,p,\nu }\)</EquationSource> </InlineEquation> version of the Heisenberg–Pauli–Weyl uncertainty principle. Furthermore, we establish three continuous uncertainty principles of concentration type. The first two principles are formulated in <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_976_Article_IEq2.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="39" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {L}_{q,p,\nu }\)</EquationSource> </InlineEquation> setting and depend on the concentration sets <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_976_Article_IEq6.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Omega \)</EquationSource> </InlineEquation> and <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_976_Article_IEq7.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Sigma \)</EquationSource> </InlineEquation>, as well as on the time function <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_976_Article_IEq8.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="16" /> </InlineMediaObject> <EquationSource Format="TEX">\(\varphi \)</EquationSource> </InlineEquation>. The third uncertainty principle is also formulated in the <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_976_Article_IEq2.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="39" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {L}_{q,p,\nu }\)</EquationSource> </InlineEquation> setting, but it depends only on the sets of concentration and is independent of the bandlimited function <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_976_Article_IEq8.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="16" /> </InlineMediaObject> <EquationSource Format="TEX">\(\varphi \)</EquationSource> </InlineEquation>. These <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_976_Article_IEq2.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="39" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {L}_{q,p,\nu }\)</EquationSource> </InlineEquation>-Donoho-Stark-type inequalities generalize the results obtained in the case <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41478_2025_976_Article_IEq12.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="71" /> </InlineMediaObject> <EquationSource Format="TEX">\(p = q = 2\)</EquationSource> </InlineEquation>.</p>

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Generalized uncertainty principles for the q-Bessel Fourier transform

  • Bochra Nefzi,
  • Ahmed Saoudi

摘要

The aim of this paper is to establish a generalization of uncertainty principles for the q-Bessel Fourier transform, \(\mathcal {F}_{q, \nu }\) introduced earlier in Dhaouadi (Bull Math Anal Appl 5:42–60, 2013) and Dhaouadi (J Inequal Pure Appl Math 7:171, 2006). More precisely, we prove an \(\mathcal {L}_{q,p,\nu }\) -local uncertainty principle for \(\mathcal {F}_{q, \nu }\) , and we derive an \(\mathcal {L}_{q,p,\nu }\) version of the Heisenberg–Pauli–Weyl uncertainty principle. Furthermore, we establish three continuous uncertainty principles of concentration type. The first two principles are formulated in \(\mathcal {L}_{q,p,\nu }\) setting and depend on the concentration sets \(\Omega \) and \(\Sigma \) , as well as on the time function \(\varphi \) . The third uncertainty principle is also formulated in the \(\mathcal {L}_{q,p,\nu }\) setting, but it depends only on the sets of concentration and is independent of the bandlimited function \(\varphi \) . These \(\mathcal {L}_{q,p,\nu }\) -Donoho-Stark-type inequalities generalize the results obtained in the case \(p = q = 2\) .