<p>The systolic area <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2197_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="31" /> </InlineMediaObject> <EquationSource Format="TEX">\(\alpha _{sys}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>α</mi> <mrow> <mi mathvariant="italic">sys</mi> </mrow> </msub> </math></EquationSource> </InlineEquation> of a nonsimply connected compact Riemannian surface (<i>M</i>,&#xa0;<i>g</i>) is defined as its area divided by the square of the systole, where the systole is equal to the length of a shortest noncontractible closed curve. The systolic inequality due to Bavard states that on the Klein bottle, the systolic area has the optimal lower bound <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2197_Article_IEq2.gif" Format="GIF" Height="26" Rendition="HTML" Resolution="72" Type="Linedraw" Width="24" /> </InlineMediaObject> <EquationSource Format="TEX">\(\frac{2\sqrt{2}}{\pi }\)</EquationSource> <EquationSource Format="MATHML"><math> <mfrac> <mrow> <mn>2</mn> <msqrt> <mn>2</mn> </msqrt> </mrow> <mi>π</mi> </mfrac> </math></EquationSource> </InlineEquation>. Bavard also constructed metrics of minimal systolic area in any given conformal class. We give an alternative proof of these results, which also yields an estimate on the systolic defect <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2197_Article_IEq3.gif" Format="GIF" Height="26" Rendition="HTML" Resolution="72" Type="Linedraw" Width="74" /> </InlineMediaObject> <EquationSource Format="TEX">\(\alpha _{sys}-\frac{2\sqrt{2}}{\pi }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>α</mi> <mrow> <mi mathvariant="italic">sys</mi> </mrow> </msub> <mo>-</mo> <mfrac> <mrow> <mn>2</mn> <msqrt> <mn>2</mn> </msqrt> </mrow> <mi>π</mi> </mfrac> </mrow> </math></EquationSource> </InlineEquation> in terms of the <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2197_Article_IEq4.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^2\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mn>2</mn> </msup> </math></EquationSource> </InlineEquation>-distance of the conformal factor to the metric which minimizes the systolic area. On the Möbius strip, we also prove similar estimates for metrics in fixed conformal classes.</p>

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Stability of Systolic Inequalities for the Möbius Strip and Klein Bottle

  • Jan Eyll

摘要

The systolic area \(\alpha _{sys}\) α sys of a nonsimply connected compact Riemannian surface (Mg) is defined as its area divided by the square of the systole, where the systole is equal to the length of a shortest noncontractible closed curve. The systolic inequality due to Bavard states that on the Klein bottle, the systolic area has the optimal lower bound \(\frac{2\sqrt{2}}{\pi }\) 2 2 π . Bavard also constructed metrics of minimal systolic area in any given conformal class. We give an alternative proof of these results, which also yields an estimate on the systolic defect \(\alpha _{sys}-\frac{2\sqrt{2}}{\pi }\) α sys - 2 2 π in terms of the \(L^2\) L 2 -distance of the conformal factor to the metric which minimizes the systolic area. On the Möbius strip, we also prove similar estimates for metrics in fixed conformal classes.