<p>Let <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\mathcal {M}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">M</mi> </math></EquationSource> </InlineEquation> be a smooth, closed and connected manifold of dimension <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(n\in \mathbb {N}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>∈</mo> <mi mathvariant="double-struck">N</mi> </mrow> </math></EquationSource> </InlineEquation>, endowed with a Riemannian metric <i>g</i>. Moreover, let <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\mathcal {B}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">B</mi> </math></EquationSource> </InlineEquation> be an <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\((n+1)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <mi>n</mi> <mo>+</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>-dimensional compact manifold with boundary equal to <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\mathcal {M}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">M</mi> </math></EquationSource> </InlineEquation>. Endow <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\mathcal {B}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">B</mi> </math></EquationSource> </InlineEquation> with a Riemannian metric <i>h</i> such that, in local coordinates <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\((x,y)\in [0,1)\times \mathcal {M}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>y</mi> <mo stretchy="false">)</mo> <mo>∈</mo> <mo stretchy="false">[</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">)</mo> <mo>×</mo> <mi mathvariant="script">M</mi> </mrow> </math></EquationSource> </InlineEquation> on the collar part of the boundary, it admits the warped product form <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(h=dx^{2}+x^{2}g(y)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>h</mi> <mo>=</mo> <mi>d</mi> <msup> <mi>x</mi> <mn>2</mn> </msup> <mo>+</mo> <msup> <mi>x</mi> <mn>2</mn> </msup> <mi>g</mi> <mrow> <mo stretchy="false">(</mo> <mi>y</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. We consider the homogeneous heat equation on <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\((\mathcal {B},h)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="script">B</mi> <mo>,</mo> <mi>h</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> and find an arbitrary long asymptotic expansion of the solutions with respect to <i>x</i> near 0. It turns out that the spectrum of the Laplacian on <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\((\mathcal {M},g)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="script">M</mi> <mo>,</mo> <mi>g</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> determines explicitly the above asymptotic expansion and vice versa.</p>

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The spectrum of the Laplacian on closed manifolds and the heat asymptotics near conical points

  • Nikolaos Roidos

摘要

Let \(\mathcal {M}\) M be a smooth, closed and connected manifold of dimension \(n\in \mathbb {N}\) n N , endowed with a Riemannian metric g. Moreover, let \(\mathcal {B}\) B be an \((n+1)\) ( n + 1 ) -dimensional compact manifold with boundary equal to \(\mathcal {M}\) M . Endow \(\mathcal {B}\) B with a Riemannian metric h such that, in local coordinates \((x,y)\in [0,1)\times \mathcal {M}\) ( x , y ) [ 0 , 1 ) × M on the collar part of the boundary, it admits the warped product form \(h=dx^{2}+x^{2}g(y)\) h = d x 2 + x 2 g ( y ) . We consider the homogeneous heat equation on \((\mathcal {B},h)\) ( B , h ) and find an arbitrary long asymptotic expansion of the solutions with respect to x near 0. It turns out that the spectrum of the Laplacian on \((\mathcal {M},g)\) ( M , g ) determines explicitly the above asymptotic expansion and vice versa.