<p>We determine the <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\ell ^p\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>ℓ</mi> <mi>p</mi> </msup> </math></EquationSource> </InlineEquation>-spectrum of the isotropic nearest-neighbor stochastic transition operator <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\mu _1\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>μ</mi> <mn>1</mn> </msub> </math></EquationSource> </InlineEquation> acting on functions on the set <i>V</i> of vertices of a semi-homogeneous tree; in the much simpler setting of homogeneous trees, the spectrum has been known for a long time. The spectrum is given by the eigenvalues of spherical functions, normalized at a reference vertex <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(v_0\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>v</mi> <mn>0</mn> </msub> </math></EquationSource> </InlineEquation>. We first show that spherical functions are boundary integrals of generalized Poisson kernels that, unlike the homogeneous setting, are not complex powers of the usual Poisson kernel. Then we compute these generalized Poisson kernels via Markov chains and their generating functions, whence we work out explicit expressions for spherical functions, that turn out to have an <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\ell ^p\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>ℓ</mi> <mi>p</mi> </msup> </math></EquationSource> </InlineEquation> behavior different from the homogeneous setting; indeed, one of them, for an appropriate choice of <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(v_0\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>v</mi> <mn>0</mn> </msub> </math></EquationSource> </InlineEquation>, belongs to <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\ell ^p\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>ℓ</mi> <mi>p</mi> </msup> </math></EquationSource> </InlineEquation> for some <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(p&lt;2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>&lt;</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>. Up to normalization, on each of the two homogeneity classes, that is, on each orbit <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(V_+\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>V</mi> <mo>+</mo> </msub> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(V_-\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>V</mi> <mo>-</mo> </msub> </math></EquationSource> </InlineEquation> of the Markov chain induced by <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\mu _1\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>μ</mi> <mn>1</mn> </msub> </math></EquationSource> </InlineEquation>, the operator <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\mu _1^2\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>μ</mi> <mn>1</mn> <mn>2</mn> </msubsup> </math></EquationSource> </InlineEquation> differs from the step-2 isotropic operator <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(\mu _2\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>μ</mi> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation> only by a shift. On the other hand, the recurrence relation associated to the semi-homogeneous <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(\mu _2\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>μ</mi> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation> is that of a polygonal graph, akin to that of <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(\mu _1\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>μ</mi> <mn>1</mn> </msub> </math></EquationSource> </InlineEquation> on a homogeneous tree. By this token, we compute the spectra of <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(\mu _1^2\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>μ</mi> <mn>1</mn> <mn>2</mn> </msubsup> </math></EquationSource> </InlineEquation> on <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(\ell ^p(V_+)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>ℓ</mi> <mi>p</mi> </msup> <mrow> <mo stretchy="false">(</mo> <msub> <mi>V</mi> <mo>+</mo> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(\ell ^p(V_-)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>ℓ</mi> <mi>p</mi> </msup> <mrow> <mo stretchy="false">(</mo> <msub> <mi>V</mi> <mo>-</mo> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, hence, by extracting square roots, the spectrum of <InlineEquation ID="IEq18"> <EquationSource Format="TEX">\(\mu _1\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>μ</mi> <mn>1</mn> </msub> </math></EquationSource> </InlineEquation> on <InlineEquation ID="IEq19"> <EquationSource Format="TEX">\(\ell ^p(V)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>ℓ</mi> <mi>p</mi> </msup> <mrow> <mo stretchy="false">(</mo> <mi>V</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> for <InlineEquation ID="IEq20"> <EquationSource Format="TEX">\(1\leqslant p &lt;\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo>⩽</mo> <mi>p</mi> <mo>&lt;</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation>. We show that this spectrum is disconnected for <i>p</i> in an interval containing 2 but connected for all other values of <i>p</i>, whereas in the homogeneous setting it is connected for every <i>p</i>.</p>

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Spherical Functions and Spectrum of the Laplacian on Semi-homogeneous Trees

  • Enrico Casadio Tarabusi,
  • Massimo A. Picardello

摘要

We determine the \(\ell ^p\) p -spectrum of the isotropic nearest-neighbor stochastic transition operator \(\mu _1\) μ 1 acting on functions on the set V of vertices of a semi-homogeneous tree; in the much simpler setting of homogeneous trees, the spectrum has been known for a long time. The spectrum is given by the eigenvalues of spherical functions, normalized at a reference vertex \(v_0\) v 0 . We first show that spherical functions are boundary integrals of generalized Poisson kernels that, unlike the homogeneous setting, are not complex powers of the usual Poisson kernel. Then we compute these generalized Poisson kernels via Markov chains and their generating functions, whence we work out explicit expressions for spherical functions, that turn out to have an \(\ell ^p\) p behavior different from the homogeneous setting; indeed, one of them, for an appropriate choice of \(v_0\) v 0 , belongs to \(\ell ^p\) p for some \(p<2\) p < 2 . Up to normalization, on each of the two homogeneity classes, that is, on each orbit \(V_+\) V + , \(V_-\) V - of the Markov chain induced by \(\mu _1\) μ 1 , the operator \(\mu _1^2\) μ 1 2 differs from the step-2 isotropic operator \(\mu _2\) μ 2 only by a shift. On the other hand, the recurrence relation associated to the semi-homogeneous \(\mu _2\) μ 2 is that of a polygonal graph, akin to that of \(\mu _1\) μ 1 on a homogeneous tree. By this token, we compute the spectra of \(\mu _1^2\) μ 1 2 on \(\ell ^p(V_+)\) p ( V + ) and \(\ell ^p(V_-)\) p ( V - ) , hence, by extracting square roots, the spectrum of \(\mu _1\) μ 1 on \(\ell ^p(V)\) p ( V ) for \(1\leqslant p <\infty \) 1 p < . We show that this spectrum is disconnected for p in an interval containing 2 but connected for all other values of p, whereas in the homogeneous setting it is connected for every p.