<p>In this paper, we consider the operator <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\Xi _{\alpha }^{\mathcal {M}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi mathvariant="normal">Ξ</mi> <mrow> <mi>α</mi> </mrow> <mi mathvariant="script">M</mi> </msubsup> </math></EquationSource> </InlineEquation> defined by <Equation ID="Equ43"> <EquationSource Format="TEX">\(\begin{aligned} \Xi _{\alpha }^{\mathcal {M}}f(x)=f'(-x)+\frac{\alpha }{x}(f(x)-f(-x))+\frac{ia}{b}xf(-x),\,\alpha \geqslant 0,\, a,b\in \mathbb {R},\,b\ne 0, \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <msubsup> <mi mathvariant="normal">Ξ</mi> <mrow> <mi>α</mi> </mrow> <mi mathvariant="script">M</mi> </msubsup> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <msup> <mi>f</mi> <mo>′</mo> </msup> <mrow> <mo stretchy="false">(</mo> <mo>-</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>+</mo> <mfrac> <mi>α</mi> <mi>x</mi> </mfrac> <mrow> <mo stretchy="false">(</mo> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>-</mo> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <mo>-</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">)</mo> </mrow> <mo>+</mo> <mfrac> <mrow> <mi mathvariant="italic">ia</mi> </mrow> <mi>b</mi> </mfrac> <mi>x</mi> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <mo>-</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> <mspace width="0.166667em" /> <mi>α</mi> <mo>⩾</mo> <mn>0</mn> <mo>,</mo> <mspace width="0.166667em" /> <mi>a</mi> <mo>,</mo> <mi>b</mi> <mo>∈</mo> <mi mathvariant="double-struck">R</mi> <mo>,</mo> <mspace width="0.166667em" /> <mi>b</mi> <mo>≠</mo> <mn>0</mn> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <i>f</i> is a differentiable function on <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\mathbb {R}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">R</mi> </math></EquationSource> </InlineEquation>. We develop an in-depth harmonic analysis associated with the operator <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\Xi _{\alpha }^{\mathcal {M}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi mathvariant="normal">Ξ</mi> <mrow> <mi>α</mi> </mrow> <mi mathvariant="script">M</mi> </msubsup> </math></EquationSource> </InlineEquation>. Firstly, we introduce and analyze the linear canonical Hartley–Bessel transform, deriving some of its fundamental properties, such as inversion formula and Plancherel formula. Secondly, we present the translation operator associated with <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\Xi _{\alpha }^{\mathcal {M}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi mathvariant="normal">Ξ</mi> <mrow> <mi>α</mi> </mrow> <mi mathvariant="script">M</mi> </msubsup> </math></EquationSource> </InlineEquation> and explore some of its key properties. Next, we derive a convolution product for this transform. Building on the previous results, we define and study the linear canonical Hartley–Bessel wavelet transform <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\mathcal {W}^{\mathcal {M}}_{\psi }\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mrow> <mi mathvariant="script">W</mi> </mrow> <mi>ψ</mi> <mi mathvariant="script">M</mi> </msubsup> </math></EquationSource> </InlineEquation> and establish its fundamental properties. Also some inequalities of this transform are proved. Finally, we define the localization operators <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\mathfrak {L}_{u,v}(\sigma )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="fraktur">L</mi> <mrow> <mi>u</mi> <mo>,</mo> <mi>v</mi> </mrow> </msub> <mrow> <mo stretchy="false">(</mo> <mi>σ</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> associated with <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\mathcal {W}^{\mathcal {M}}_{\psi }\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mrow> <mi mathvariant="script">W</mi> </mrow> <mi>ψ</mi> <mi mathvariant="script">M</mi> </msubsup> </math></EquationSource> </InlineEquation> and we study the boundedness and compactness of these operators and establish a trace formula.</p>

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Some results connected to the linear canonical Hartley–Bessel wavelet transform

  • Khaled Hleili,
  • Manel Hleili

摘要

In this paper, we consider the operator \(\Xi _{\alpha }^{\mathcal {M}}\) Ξ α M defined by \(\begin{aligned} \Xi _{\alpha }^{\mathcal {M}}f(x)=f'(-x)+\frac{\alpha }{x}(f(x)-f(-x))+\frac{ia}{b}xf(-x),\,\alpha \geqslant 0,\, a,b\in \mathbb {R},\,b\ne 0, \end{aligned}\) Ξ α M f ( x ) = f ( - x ) + α x ( f ( x ) - f ( - x ) ) + ia b x f ( - x ) , α 0 , a , b R , b 0 , where f is a differentiable function on \(\mathbb {R}\) R . We develop an in-depth harmonic analysis associated with the operator \(\Xi _{\alpha }^{\mathcal {M}}\) Ξ α M . Firstly, we introduce and analyze the linear canonical Hartley–Bessel transform, deriving some of its fundamental properties, such as inversion formula and Plancherel formula. Secondly, we present the translation operator associated with \(\Xi _{\alpha }^{\mathcal {M}}\) Ξ α M and explore some of its key properties. Next, we derive a convolution product for this transform. Building on the previous results, we define and study the linear canonical Hartley–Bessel wavelet transform \(\mathcal {W}^{\mathcal {M}}_{\psi }\) W ψ M and establish its fundamental properties. Also some inequalities of this transform are proved. Finally, we define the localization operators \(\mathfrak {L}_{u,v}(\sigma )\) L u , v ( σ ) associated with \(\mathcal {W}^{\mathcal {M}}_{\psi }\) W ψ M and we study the boundedness and compactness of these operators and establish a trace formula.