<p>In this contribution we deal with pairs of symmetric linear functionals <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(({\textbf {u}} ,{\textbf {v}} )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="bold">u</mi> <mo>,</mo> <mi mathvariant="bold">v</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> such that the corresponding sequences of monic orthogonal polynomials <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\{P_n(x;{\textbf {u}} )\}_{n\ge 0}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mrow> <mo stretchy="false">{</mo> <msub> <mi>P</mi> <mi>n</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>;</mo> <mi mathvariant="bold">u</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">}</mo> </mrow> <mrow> <mi>n</mi> <mo>≥</mo> <mn>0</mn> </mrow> </msub> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\{ P_n(x;{\textbf {v}} )\}_{n\ge 0}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mrow> <mo stretchy="false">{</mo> <msub> <mi>P</mi> <mi>n</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>;</mo> <mi mathvariant="bold">v</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">}</mo> </mrow> <mrow> <mi>n</mi> <mo>≥</mo> <mn>0</mn> </mrow> </msub> </math></EquationSource> </InlineEquation> are related by <Equation ID="Equ31"> <EquationSource Format="TEX">\( \frac{T_{\mu }P_{n+1}(x;{\textbf {u}} )}{\mu _{n+1}}=P_n(x;{\textbf {v}} )-\tau _{n-1}P_{n-2}(x;{\textbf {v}} ),\quad \tau _{n-1}\ne 0,\quad n\ge 2. \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mfrac> <mrow> <msub> <mi>T</mi> <mi>μ</mi> </msub> <msub> <mi>P</mi> <mrow> <mi>n</mi> <mo>+</mo> <mn>1</mn> </mrow> </msub> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>;</mo> <mi mathvariant="bold">u</mi> <mo stretchy="false">)</mo> </mrow> </mrow> <msub> <mi>μ</mi> <mrow> <mi>n</mi> <mo>+</mo> <mn>1</mn> </mrow> </msub> </mfrac> <mo>=</mo> <msub> <mi>P</mi> <mi>n</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>;</mo> <mi mathvariant="bold">v</mi> <mo stretchy="false">)</mo> </mrow> <mo>-</mo> <msub> <mi>τ</mi> <mrow> <mi>n</mi> <mo>-</mo> <mn>1</mn> </mrow> </msub> <msub> <mi>P</mi> <mrow> <mi>n</mi> <mo>-</mo> <mn>2</mn> </mrow> </msub> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>;</mo> <mi mathvariant="bold">v</mi> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> <mspace width="1em" /> <msub> <mi>τ</mi> <mrow> <mi>n</mi> <mo>-</mo> <mn>1</mn> </mrow> </msub> <mo>≠</mo> <mn>0</mn> <mo>,</mo> <mspace width="1em" /> <mi>n</mi> <mo>≥</mo> <mn>2</mn> <mo>.</mo> </mrow> </math></EquationSource> </Equation>Here <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(T_{\mu }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>T</mi> <mi>μ</mi> </msub> </math></EquationSource> </InlineEquation> is the standard Dunkl operator in one variable. Such a pair of linear functionals is said to be a symmetric <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(T_{\mu }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>T</mi> <mi>μ</mi> </msub> </math></EquationSource> </InlineEquation>-coherent pair of the second kind. We give a necessary and sufficient condition in order for a pair of symmetric linear functionals to be a <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(T_{\mu }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>T</mi> <mi>μ</mi> </msub> </math></EquationSource> </InlineEquation>-coherent pair of the second kind. We describe all of such linear functionals. In particular, we focus our attention on the companions of <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(T_{\mu }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>T</mi> <mi>μ</mi> </msub> </math></EquationSource> </InlineEquation>-classical linear functionals (Generalized Hermite and Generalized Gegenbauer).</p>

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Dunkl symmetric coherent pairs of the second kind of positive measures

  • Francisco Marcellán,
  • Judit Mínguez Ceniceros

摘要

In this contribution we deal with pairs of symmetric linear functionals \(({\textbf {u}} ,{\textbf {v}} )\) ( u , v ) such that the corresponding sequences of monic orthogonal polynomials \(\{P_n(x;{\textbf {u}} )\}_{n\ge 0}\) { P n ( x ; u ) } n 0 and \(\{ P_n(x;{\textbf {v}} )\}_{n\ge 0}\) { P n ( x ; v ) } n 0 are related by \( \frac{T_{\mu }P_{n+1}(x;{\textbf {u}} )}{\mu _{n+1}}=P_n(x;{\textbf {v}} )-\tau _{n-1}P_{n-2}(x;{\textbf {v}} ),\quad \tau _{n-1}\ne 0,\quad n\ge 2. \) T μ P n + 1 ( x ; u ) μ n + 1 = P n ( x ; v ) - τ n - 1 P n - 2 ( x ; v ) , τ n - 1 0 , n 2 . Here \(T_{\mu }\) T μ is the standard Dunkl operator in one variable. Such a pair of linear functionals is said to be a symmetric \(T_{\mu }\) T μ -coherent pair of the second kind. We give a necessary and sufficient condition in order for a pair of symmetric linear functionals to be a \(T_{\mu }\) T μ -coherent pair of the second kind. We describe all of such linear functionals. In particular, we focus our attention on the companions of \(T_{\mu }\) T μ -classical linear functionals (Generalized Hermite and Generalized Gegenbauer).