<p>The local topology of singular points in analytic spaces is known, by work of Milnor and others, to be determined by its link <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40590_2025_761_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(L_0\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>L</mi> <mn>0</mn> </msub> </math></EquationSource> </InlineEquation>. In this work, we look at holomorphic map-germs <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40590_2025_761_Article_IEq2.gif" Format="GIF" Height="25" Rendition="HTML" Resolution="72" Type="Linedraw" Width="109" /> </InlineMediaObject> <EquationSource Format="TEX">\((X,{\underline{0}}) \buildrel {f}\over {\rightarrow } ({{\mathbb {C}}},0)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">(</mo> <mi>X</mi> <mo>,</mo> <munder> <mn>0</mn> <mo>̲</mo> </munder> <mo stretchy="false">)</mo> </mrow> <mover> <mo stretchy="false">→</mo> <mi>f</mi> </mover> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="double-struck">C</mi> <mo>,</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> where <i>X</i> is an arbitrary reduced and equidimensional complex analytic space in some <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40590_2025_761_Article_IEq3.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="24" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathbb {C}}^m\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">C</mi> </mrow> <mi>m</mi> </msup> </math></EquationSource> </InlineEquation>. We compare the topology of the link <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40590_2025_761_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(L_0\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>L</mi> <mn>0</mn> </msub> </math></EquationSource> </InlineEquation> with that of the boundary of a local non-critical level, i.e., with the boundary of its Milnor fiber <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40590_2025_761_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(F_t\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>F</mi> <mi>t</mi> </msub> </math></EquationSource> </InlineEquation>. We study how the topology of the boundary <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40590_2025_761_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="29" /> </InlineMediaObject> <EquationSource Format="TEX">\(\partial F_t\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>∂</mi> <msub> <mi>F</mi> <mi>t</mi> </msub> </mrow> </math></EquationSource> </InlineEquation> changes as the non-critical level degenerates to the critical one.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Vanishing and nearby boundary cycles of complex non-isolated singularities

  • Marcelo Aguilar,
  • Aurelio Menegon,
  • José Seade

摘要

The local topology of singular points in analytic spaces is known, by work of Milnor and others, to be determined by its link \(L_0\) L 0 . In this work, we look at holomorphic map-germs \((X,{\underline{0}}) \buildrel {f}\over {\rightarrow } ({{\mathbb {C}}},0)\) ( X , 0 ̲ ) f ( C , 0 ) where X is an arbitrary reduced and equidimensional complex analytic space in some \({\mathbb {C}}^m\) C m . We compare the topology of the link \(L_0\) L 0 with that of the boundary of a local non-critical level, i.e., with the boundary of its Milnor fiber \(F_t\) F t . We study how the topology of the boundary \(\partial F_t\) F t changes as the non-critical level degenerates to the critical one.