<p>Ruberman constructed families <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\{g_n\vert n \in \mathbb {N}\} \subset \mathcal {R}^+ (M)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">{</mo> <msub> <mi>g</mi> <mi>n</mi> </msub> <mo stretchy="false">|</mo> <mi>n</mi> <mo>∈</mo> <mi mathvariant="double-struck">N</mi> <mo stretchy="false">}</mo> </mrow> <mo>⊂</mo> <msup> <mrow> <mi mathvariant="script">R</mi> </mrow> <mo>+</mo> </msup> <mrow> <mo stretchy="false">(</mo> <mi>M</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> of metrics of positive scalar curvature on certain 4-manifolds which are concordant but lie in different path components of <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\mathcal {R}^+ (M)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mrow> <mi mathvariant="script">R</mi> </mrow> <mo>+</mo> </msup> <mrow> <mo stretchy="false">(</mo> <mi>M</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. We prove a cancellation result along the following lines. For each closed manifold <i>N</i>, there is a map <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\nu _N: \mathcal {R}^+ (M) \rightarrow \mathcal {R}^+ (M \times N)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>ν</mi> <mi>N</mi> </msub> <mo>:</mo> <msup> <mrow> <mi mathvariant="script">R</mi> </mrow> <mo>+</mo> </msup> <mrow> <mo stretchy="false">(</mo> <mi>M</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">→</mo> <msup> <mrow> <mi mathvariant="script">R</mi> </mrow> <mo>+</mo> </msup> <mrow> <mo stretchy="false">(</mo> <mi>M</mi> <mo>×</mo> <mi>N</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, well-defined up to homotopy, that takes the product with <i>N</i>. We prove that when <i>N</i> has positive dimension <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\nu _N\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>ν</mi> <mi>N</mi> </msub> </math></EquationSource> </InlineEquation> takes all metrics of Ruberman’s family to the same path component. This is trivial when <i>N</i> has a psc metric and follows from pseudoisotopy theory when <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\dim (N) \ge 3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>dim</mo> <mo stretchy="false">(</mo> <mi>N</mi> <mo stretchy="false">)</mo> <mo>≥</mo> <mn>3</mn> </mrow> </math></EquationSource> </InlineEquation>. More generally, we give easily checkable conditions on diffeomorphisms <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(f:M \rightarrow M\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>f</mi> <mo>:</mo> <mi>M</mi> <mo stretchy="false">→</mo> <mi>M</mi> </mrow> </math></EquationSource> </InlineEquation> of 1-connected 4-manifolds which guarantee that for each closed <i>N</i> and each <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(g \in \mathcal {R}^+ (M)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>g</mi> <mo>∈</mo> <msup> <mrow> <mi mathvariant="script">R</mi> </mrow> <mo>+</mo> </msup> <mrow> <mo stretchy="false">(</mo> <mi>M</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, the metrics <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\nu _N (g)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>ν</mi> <mi>N</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>g</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\nu _N (f^* g)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>ν</mi> <mi>N</mi> </msub> <mrow> <mo stretchy="false">(</mo> <msup> <mi>f</mi> <mo>∗</mo> </msup> <mi>g</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> lie in the same path component of <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\mathcal {R}^+ (M \times N)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mrow> <mi mathvariant="script">R</mi> </mrow> <mo>+</mo> </msup> <mrow> <mo stretchy="false">(</mo> <mi>M</mi> <mo>×</mo> <mi>N</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. The conditions are (A) the cobordism class of the mapping torus <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\([T(f)] \in \Omega _5^\textrm{SO}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">[</mo> <mi>T</mi> <mrow> <mo stretchy="false">(</mo> <mi>f</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">]</mo> </mrow> <mo>∈</mo> <msubsup> <mi mathvariant="normal">Ω</mi> <mn>5</mn> <mtext>SO</mtext> </msubsup> </mrow> </math></EquationSource> </InlineEquation> vanishes and (B) the induced map <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(f^*: H^2 (M;\mathbb {R}) \rightarrow H^2(M;\mathbb {R})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>f</mi> <mo>∗</mo> </msup> <mo>:</mo> <msup> <mi>H</mi> <mn>2</mn> </msup> <mrow> <mo stretchy="false">(</mo> <mi>M</mi> <mo>;</mo> <mi mathvariant="double-struck">R</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">→</mo> <msup> <mi>H</mi> <mn>2</mn> </msup> <mrow> <mo stretchy="false">(</mo> <mi>M</mi> <mo>;</mo> <mi mathvariant="double-struck">R</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> belongs to the unit component of <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(\textrm{Aut}(I_M)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mtext>Aut</mtext> <mo stretchy="false">(</mo> <msub> <mi>I</mi> <mi>M</mi> </msub> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>, the orthogonal group of the intersection form of <i>M</i>. Depending on whether <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(\dim (N)=1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>dim</mo> <mo stretchy="false">(</mo> <mi>N</mi> <mo stretchy="false">)</mo> <mo>=</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> or <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(\dim (N) \ge 2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>dim</mo> <mo stretchy="false">(</mo> <mi>N</mi> <mo stretchy="false">)</mo> <mo>≥</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation> and on whether or not <i>M</i> is spin, various combinations of (A) and (B) are needed. The proof uses rigidity properties for the diffeomorphism action on <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(\mathcal {R}^+ (M)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mrow> <mi mathvariant="script">R</mi> </mrow> <mo>+</mo> </msup> <mrow> <mo stretchy="false">(</mo> <mi>M</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> for high–dimensional <i>M</i>, which in the necessary generality were established by Frenck and Bantje. These rigidity properties reduce the problem to a calculation of the homotopy group <InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(\pi _1 (\textrm{MTSO}(4))\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>π</mi> <mn>1</mn> </msub> <mrow> <mo stretchy="false">(</mo> <mtext>MTSO</mtext> <mrow> <mo stretchy="false">(</mo> <mn>4</mn> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> of the Madsen–Tillmann spectrum which we also carry out. Recently, Auckly and Ruberman exhibited examples of elements in higher homotopy groups of <InlineEquation ID="IEq18"> <EquationSource Format="TEX">\(\mathcal {R}^+(M^4)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mrow> <mi mathvariant="script">R</mi> </mrow> <mo>+</mo> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mi>M</mi> <mn>4</mn> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> for certain <i>M</i>. Using the same method, we also prove that these elements lie in the kernel of the induced map <InlineEquation ID="IEq19"> <EquationSource Format="TEX">\((\nu _N)_*\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow> <mo stretchy="false">(</mo> <msub> <mi>ν</mi> <mi>N</mi> </msub> <mo stretchy="false">)</mo> </mrow> <mrow> <mrow /> <mo>∗</mo> </mrow> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation> on rational homotopy.</p>

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Cancellation properties for exotic 4-dimensional positive scalar curvature metrics

  • Johannes Ebert

摘要

Ruberman constructed families \(\{g_n\vert n \in \mathbb {N}\} \subset \mathcal {R}^+ (M)\) { g n | n N } R + ( M ) of metrics of positive scalar curvature on certain 4-manifolds which are concordant but lie in different path components of \(\mathcal {R}^+ (M)\) R + ( M ) . We prove a cancellation result along the following lines. For each closed manifold N, there is a map \(\nu _N: \mathcal {R}^+ (M) \rightarrow \mathcal {R}^+ (M \times N)\) ν N : R + ( M ) R + ( M × N ) , well-defined up to homotopy, that takes the product with N. We prove that when N has positive dimension \(\nu _N\) ν N takes all metrics of Ruberman’s family to the same path component. This is trivial when N has a psc metric and follows from pseudoisotopy theory when \(\dim (N) \ge 3\) dim ( N ) 3 . More generally, we give easily checkable conditions on diffeomorphisms \(f:M \rightarrow M\) f : M M of 1-connected 4-manifolds which guarantee that for each closed N and each \(g \in \mathcal {R}^+ (M)\) g R + ( M ) , the metrics \(\nu _N (g)\) ν N ( g ) and \(\nu _N (f^* g)\) ν N ( f g ) lie in the same path component of \(\mathcal {R}^+ (M \times N)\) R + ( M × N ) . The conditions are (A) the cobordism class of the mapping torus \([T(f)] \in \Omega _5^\textrm{SO}\) [ T ( f ) ] Ω 5 SO vanishes and (B) the induced map \(f^*: H^2 (M;\mathbb {R}) \rightarrow H^2(M;\mathbb {R})\) f : H 2 ( M ; R ) H 2 ( M ; R ) belongs to the unit component of \(\textrm{Aut}(I_M)\) Aut ( I M ) , the orthogonal group of the intersection form of M. Depending on whether \(\dim (N)=1\) dim ( N ) = 1 or \(\dim (N) \ge 2\) dim ( N ) 2 and on whether or not M is spin, various combinations of (A) and (B) are needed. The proof uses rigidity properties for the diffeomorphism action on \(\mathcal {R}^+ (M)\) R + ( M ) for high–dimensional M, which in the necessary generality were established by Frenck and Bantje. These rigidity properties reduce the problem to a calculation of the homotopy group \(\pi _1 (\textrm{MTSO}(4))\) π 1 ( MTSO ( 4 ) ) of the Madsen–Tillmann spectrum which we also carry out. Recently, Auckly and Ruberman exhibited examples of elements in higher homotopy groups of \(\mathcal {R}^+(M^4)\) R + ( M 4 ) for certain M. Using the same method, we also prove that these elements lie in the kernel of the induced map \((\nu _N)_*\) ( ν N ) on rational homotopy.