<p>We present a new and simpler proof of the fact that any Lagrangian <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40316_2024_238_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="31" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathbb {R}}P^2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="double-struck">R</mi> <msup> <mi>P</mi> <mn>2</mn> </msup> </mrow> </math></EquationSource> </InlineEquation> in <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40316_2024_238_Article_IEq4.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="50" /> </InlineMediaObject> <EquationSource Format="TEX">\(T^*{\mathbb {R}}P^2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>T</mi> <mo>∗</mo> </msup> <mi mathvariant="double-struck">R</mi> <msup> <mi>P</mi> <mn>2</mn> </msup> </mrow> </math></EquationSource> </InlineEquation> is Hamiltonian isotopic to the zero section. Our proof mirrors the one given by Li and Wu for the Hamiltonian uniqueness of Lagrangians in <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40316_2024_238_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="38" /> </InlineMediaObject> <EquationSource Format="TEX">\(T^*S^2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>T</mi> <mo>∗</mo> </msup> <msup> <mi>S</mi> <mn>2</mn> </msup> </mrow> </math></EquationSource> </InlineEquation>, using surgery to turn Lagrangian spheres into symplectic ones. The main novel contribution is a detailed proof of the folklore fact that the complement of a symplectic quadric in <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40316_2024_238_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="32" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathbb {C}}P^2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="double-struck">C</mi> <msup> <mi>P</mi> <mn>2</mn> </msup> </mrow> </math></EquationSource> </InlineEquation> can be identified with the unit cotangent disc bundle of <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40316_2024_238_Article_IEq7.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="31" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathbb {R}}P^2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="double-struck">R</mi> <msup> <mi>P</mi> <mn>2</mn> </msup> </mrow> </math></EquationSource> </InlineEquation>.</p>

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Uniqueness of Lagrangians in \(T^*{\mathbb {R}}P^2\)

  • Nikolas Adaloglou

摘要

We present a new and simpler proof of the fact that any Lagrangian \({\mathbb {R}}P^2\) R P 2 in \(T^*{\mathbb {R}}P^2\) T R P 2 is Hamiltonian isotopic to the zero section. Our proof mirrors the one given by Li and Wu for the Hamiltonian uniqueness of Lagrangians in \(T^*S^2\) T S 2 , using surgery to turn Lagrangian spheres into symplectic ones. The main novel contribution is a detailed proof of the folklore fact that the complement of a symplectic quadric in \({\mathbb {C}}P^2\) C P 2 can be identified with the unit cotangent disc bundle of \({\mathbb {R}}P^2\) R P 2 .