<p>We study the Dirichlet dynamical zeta function <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13_2025_2141_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="42" /> </InlineMediaObject> <EquationSource Format="TEX">\(\eta _D(s)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>η</mi> <mi>D</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>s</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> for billiard flow corresponding to several strictly convex disjoint obstacles. For large <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13_2025_2141_Article_IEq2.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="33" /> </InlineMediaObject> <EquationSource Format="TEX">\({{\,\textrm{Re}\,}}s\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mspace width="0.166667em" /> <mtext>Re</mtext> <mspace width="0.166667em" /> </mrow> <mi>s</mi> </mrow> </math></EquationSource> </InlineEquation>, we have <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13_2025_2141_Article_IEq3.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="218" /> </InlineMediaObject> <EquationSource Format="TEX">\(\eta _D(s) =\sum _{n= 1}^{\infty } a_n e^{-\lambda _n s}, \, a_n \in {\mathbb {R}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>η</mi> <mi>D</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>s</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <msubsup> <mo>∑</mo> <mrow> <mi>n</mi> <mo>=</mo> <mn>1</mn> </mrow> <mi>∞</mi> </msubsup> <msub> <mi>a</mi> <mi>n</mi> </msub> <msup> <mi>e</mi> <mrow> <mo>-</mo> <msub> <mi>λ</mi> <mi>n</mi> </msub> <mi>s</mi> </mrow> </msup> <mo>,</mo> <mspace width="0.166667em" /> <msub> <mi>a</mi> <mi>n</mi> </msub> <mo>∈</mo> <mi mathvariant="double-struck">R</mi> </mrow> </math></EquationSource> </InlineEquation>, and <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13_2025_2141_Article_IEq4.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="23" /> </InlineMediaObject> <EquationSource Format="TEX">\(\eta _D\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>η</mi> <mi>D</mi> </msub> </math></EquationSource> </InlineEquation> admits a meromorphic continuation to <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13_2025_2141_Article_IEq5.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathbb {C}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">C</mi> </math></EquationSource> </InlineEquation>. We obtain some conditions of the frequencies <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13_2025_2141_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(\lambda _n\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>λ</mi> <mi>n</mi> </msub> </math></EquationSource> </InlineEquation> and some sums of coefficients <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13_2025_2141_Article_IEq7.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(a_n\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>a</mi> <mi>n</mi> </msub> </math></EquationSource> </InlineEquation> which imply that <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13_2025_2141_Article_IEq4.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="23" /> </InlineMediaObject> <EquationSource Format="TEX">\(\eta _D\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>η</mi> <mi>D</mi> </msub> </math></EquationSource> </InlineEquation> cannot be prolonged as an entire function.</p>

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Dirichlet dynamical zeta function for billiard flow

  • Vesselin Petkov

摘要

We study the Dirichlet dynamical zeta function \(\eta _D(s)\) η D ( s ) for billiard flow corresponding to several strictly convex disjoint obstacles. For large \({{\,\textrm{Re}\,}}s\) Re s , we have \(\eta _D(s) =\sum _{n= 1}^{\infty } a_n e^{-\lambda _n s}, \, a_n \in {\mathbb {R}}\) η D ( s ) = n = 1 a n e - λ n s , a n R , and \(\eta _D\) η D admits a meromorphic continuation to \({\mathbb {C}}\) C . We obtain some conditions of the frequencies \(\lambda _n\) λ n and some sums of coefficients \(a_n\) a n which imply that \(\eta _D\) η D cannot be prolonged as an entire function.