<p>We study the deformation theory of the Fano scheme <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\textrm{F}=\textrm{F}(\textrm{X})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mtext>F</mtext> <mo>=</mo> <mtext>F</mtext> <mo stretchy="false">(</mo> <mtext>X</mtext> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> of lines on a cubic <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\textrm{X}\)</EquationSource> <EquationSource Format="MATHML"><math> <mtext>X</mtext> </math></EquationSource> </InlineEquation> of dimension <i>d</i> with only finitely many singularities. By taking the relative Fano scheme, we define a morphism <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\eta :\mathcal {D}_{\textrm{X}}\rightarrow \mathcal {D}_{\textrm{F}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>η</mi> <mo>:</mo> <msub> <mi mathvariant="script">D</mi> <mtext>X</mtext> </msub> <mo stretchy="false">→</mo> <msub> <mi mathvariant="script">D</mi> <mtext>F</mtext> </msub> </mrow> </math></EquationSource> </InlineEquation> of the local moduli functors associated to <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\textrm{X}\)</EquationSource> <EquationSource Format="MATHML"><math> <mtext>X</mtext> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\textrm{F}\)</EquationSource> <EquationSource Format="MATHML"><math> <mtext>F</mtext> </math></EquationSource> </InlineEquation>, respectively. We show that for <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(d\geqslant 5\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>d</mi> <mo>⩾</mo> <mn>5</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\eta \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>η</mi> </math></EquationSource> </InlineEquation> yields an isomorphism on first-order deformations; in particular, <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\eta \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>η</mi> </math></EquationSource> </InlineEquation> is an isomorphism whenever <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\textrm{H}^{0}(\Theta _{\textrm{X}})=0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mtext>H</mtext> <mn>0</mn> </msup> <mrow> <mo stretchy="false">(</mo> <msub> <mi mathvariant="normal">Θ</mi> <mtext>X</mtext> </msub> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>.</p>

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Deformations of the Fano scheme of a cubic

  • Samuel Stark

摘要

We study the deformation theory of the Fano scheme \(\textrm{F}=\textrm{F}(\textrm{X})\) F = F ( X ) of lines on a cubic \(\textrm{X}\) X of dimension d with only finitely many singularities. By taking the relative Fano scheme, we define a morphism \(\eta :\mathcal {D}_{\textrm{X}}\rightarrow \mathcal {D}_{\textrm{F}}\) η : D X D F of the local moduli functors associated to \(\textrm{X}\) X and \(\textrm{F}\) F , respectively. We show that for \(d\geqslant 5\) d 5 , \(\eta \) η yields an isomorphism on first-order deformations; in particular, \(\eta \) η is an isomorphism whenever \(\textrm{H}^{0}(\Theta _{\textrm{X}})=0\) H 0 ( Θ X ) = 0 .