Diffeomorphisms of discs Oscar Randal-Williams Smoothing theory M a - - PowerPoint PPT Presentation

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Diffeomorphisms of discs Oscar Randal-Williams Smoothing theory M a - - PowerPoint PPT Presentation

Diffeomorphisms of discs Oscar Randal-Williams Smoothing theory M a topological d -manifold, maybe with smooth boundary M S m ( M ) = { space of smooth structures on M , fixed near M } (space interpreted liberally). 1 Smoothing


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Diffeomorphisms of discs

Oscar Randal-Williams

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Smoothing theory

M a topological d-manifold, maybe with smooth boundary ∂M Sm(M) = { space of smooth structures on M, fixed near ∂M } (“space” interpreted liberally).

1

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Smoothing theory

M a topological d-manifold, maybe with smooth boundary ∂M Sm(M) = { space of smooth structures on M, fixed near ∂M } (“space” interpreted liberally). Recording germs of smooth structure near each point gives a map Sm(M) − → Γ∂(Sm(TM) → M) (the space of sections of the bundle with fibre Sm(TmM) ∼ = Sm(Rd))

1

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Smoothing theory

M a topological d-manifold, maybe with smooth boundary ∂M Sm(M) = { space of smooth structures on M, fixed near ∂M } (“space” interpreted liberally). Recording germs of smooth structure near each point gives a map Sm(M) − → Γ∂(Sm(TM) → M) (the space of sections of the bundle with fibre Sm(TmM) ∼ = Sm(Rd))

  • Theorem. [Hirsch–Mazur ’74, Kirby–Siebenmann ’77]

For d = 4 this map is a homotopy equivalence.

1

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Smoothing theory

M a topological d-manifold, maybe with smooth boundary ∂M Sm(M) = { space of smooth structures on M, fixed near ∂M } (“space” interpreted liberally). Recording germs of smooth structure near each point gives a map Sm(M) − → Γ∂(Sm(TM) → M) (the space of sections of the bundle with fibre Sm(TmM) ∼ = Sm(Rd))

  • Theorem. [Hirsch–Mazur ’74, Kirby–Siebenmann ’77]

For d = 4 this map is a homotopy equivalence. Homeo∂(M) acts on Sm(M), giving Sm(M) ∼ =

  • [W]

Homeo∂(W)/Diff∂(W) Similarly, Sm(Rd) ∼ = Homeo(Rd)/Diff(Rd)

1

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A consequence of smoothing theory

Write Top(d) := Homeo(Rd). By linearising have Diff(Rd) ≃ O(d), so Sm(Rd) ≃ Top(d)/O(d).

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A consequence of smoothing theory

Write Top(d) := Homeo(Rd). By linearising have Diff(Rd) ≃ O(d), so Sm(Rd) ≃ Top(d)/O(d). Applied to Dd, d = 4, smoothing theory gives a map Homeo∂(Dd)/Diff∂(Dd) − → Γ∂(Sm(TDd) → Dd) = map∂(Dd, Top(d)/O(d)) which is a homotopy equivalence to the path components it hits.

2

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A consequence of smoothing theory

Write Top(d) := Homeo(Rd). By linearising have Diff(Rd) ≃ O(d), so Sm(Rd) ≃ Top(d)/O(d). Applied to Dd, d = 4, smoothing theory gives a map Homeo∂(Dd)/Diff∂(Dd) − → Γ∂(Sm(TDd) → Dd) = map∂(Dd, Top(d)/O(d)) which is a homotopy equivalence to the path components it hits. The Alexander trick Homeo∂(Dd) ≃ ∗ implies BDiff∂(Dd) ≃ Ωd

0Top(d)/O(d)

(Morlet)

  • r if you prefer

Diff∂(Dd) ≃ Ωd+1Top(d)/O(d).

2

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A consequence of smoothing theory

Write Top(d) := Homeo(Rd). By linearising have Diff(Rd) ≃ O(d), so Sm(Rd) ≃ Top(d)/O(d). Applied to Dd, d = 4, smoothing theory gives a map Homeo∂(Dd)/Diff∂(Dd) − → Γ∂(Sm(TDd) → Dd) = map∂(Dd, Top(d)/O(d)) which is a homotopy equivalence to the path components it hits. The Alexander trick Homeo∂(Dd) ≃ ∗ implies BDiff∂(Dd) ≃ Ωd

0Top(d)/O(d)

(Morlet)

  • r if you prefer

Diff∂(Dd) ≃ Ωd+1Top(d)/O(d). O(d) is “well understood” so Diff∂(Dd) and Top(d) are equidifficult. But Diff∂(Dd) is more approachable: can use smoothness.

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What do we know?

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The theorem of Farrell and Hsiang

The classical approach to studying Diff∂(M) breaks up as

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The theorem of Farrell and Hsiang

The classical approach to studying Diff∂(M) breaks up as

  • 1. Space of homotopy self-equivalences hAut∂(M)

analysed by homotopy theory.

3

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The theorem of Farrell and Hsiang

The classical approach to studying Diff∂(M) breaks up as

  • 1. Space of homotopy self-equivalences hAut∂(M)

analysed by homotopy theory.

  • 2. Comparison hAut∂(M)/

Diff ∂(M) with “block-diffeomorphisms” analysed by surgery theory.

3

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The theorem of Farrell and Hsiang

The classical approach to studying Diff∂(M) breaks up as

  • 1. Space of homotopy self-equivalences hAut∂(M)

analysed by homotopy theory.

  • 2. Comparison hAut∂(M)/

Diff ∂(M) with “block-diffeomorphisms” analysed by surgery theory.

  • 3. Comparison

Diff ∂(M)/Diff ∂(M) with diffeomorphisms analysed by pseudoisotopy theory (and hence K-theory), but

  • nly valid in the “pseudoisotopy stable range”.

3

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The theorem of Farrell and Hsiang

The classical approach to studying Diff∂(M) breaks up as

  • 1. Space of homotopy self-equivalences hAut∂(M)

analysed by homotopy theory.

  • 2. Comparison hAut∂(M)/

Diff ∂(M) with “block-diffeomorphisms” analysed by surgery theory.

  • 3. Comparison

Diff ∂(M)/Diff ∂(M) with diffeomorphisms analysed by pseudoisotopy theory (and hence K-theory), but

  • nly valid in the “pseudoisotopy stable range”.

[Igusa ’84]: this is at least min( d−7

2 , d−4 3 ) ∼ d 3 . 3

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The theorem of Farrell and Hsiang

The classical approach to studying Diff∂(M) breaks up as

  • 1. Space of homotopy self-equivalences hAut∂(M)

analysed by homotopy theory.

  • 2. Comparison hAut∂(M)/

Diff ∂(M) with “block-diffeomorphisms” analysed by surgery theory.

  • 3. Comparison

Diff ∂(M)/Diff ∂(M) with diffeomorphisms analysed by pseudoisotopy theory (and hence K-theory), but

  • nly valid in the “pseudoisotopy stable range”.

[Igusa ’84]: this is at least min( d−7

2 , d−4 3 ) ∼ d 3 .

[RW ’17]: it is at most d − 2.

3

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The theorem of Farrell and Hsiang

The classical approach to studying Diff∂(M) breaks up as

  • 1. Space of homotopy self-equivalences hAut∂(M)

analysed by homotopy theory.

  • 2. Comparison hAut∂(M)/

Diff ∂(M) with “block-diffeomorphisms” analysed by surgery theory.

  • 3. Comparison

Diff ∂(M)/Diff ∂(M) with diffeomorphisms analysed by pseudoisotopy theory (and hence K-theory), but

  • nly valid in the “pseudoisotopy stable range”.

[Igusa ’84]: this is at least min( d−7

2 , d−4 3 ) ∼ d 3 .

[RW ’17]: it is at most d − 2.

  • Theorem. [Farrell–Hsiang ’78]

π∗(BDiff∂(Dd)) ⊗ Q =

  • d even

Q[4] ⊕ Q[8] ⊕ Q[12] ⊕ · · · d odd in the pseudoisotopy stable range for d (so certainly for ∗ d

3 ). 3

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The theorems of Watanabe

  • Theorem. [Watanabe ’09]

For 2n + 1 ≥ 5 and r ≥ 2 there is a surjection π(2r)(2n)(BDiff∂(D2n+1)) ⊗ Q ։ Aodd

r 4

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The theorems of Watanabe

  • Theorem. [Watanabe ’09]

For 2n + 1 ≥ 5 and r ≥ 2 there is a surjection π(2r)(2n)(BDiff∂(D2n+1)) ⊗ Q ։ Aodd

r

where

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The theorems of Watanabe

  • Theorem. [Watanabe ’09]

For 2n + 1 ≥ 5 and r ≥ 2 there is a surjection π(2r)(2n)(BDiff∂(D2n+1)) ⊗ Q ։ Aodd

r

where has dim(Aodd

r

) = 1, 1, 1, 2, 2, 3, 4, 5, 6, 8, 9, . . .

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The theorems of Watanabe

  • Theorem. [Watanabe ’09]

For 2n + 1 ≥ 5 and r ≥ 2 there is a surjection π(2r)(2n)(BDiff∂(D2n+1)) ⊗ Q ։ Aodd

r

where has dim(Aodd

r

) = 1, 1, 1, 2, 2, 3, 4, 5, 6, 8, 9, . . .

  • Theorem. [Watanabe ’18]

There is a surjection πr(BDiff∂(D4)) ⊗ Q ։ Aeven

r 4

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The theorems of Watanabe

  • Theorem. [Watanabe ’09]

For 2n + 1 ≥ 5 and r ≥ 2 there is a surjection π(2r)(2n)(BDiff∂(D2n+1)) ⊗ Q ։ Aodd

r

where has dim(Aodd

r

) = 1, 1, 1, 2, 2, 3, 4, 5, 6, 8, 9, . . .

  • Theorem. [Watanabe ’18]

There is a surjection πr(BDiff∂(D4)) ⊗ Q ։ Aeven

r

where dim(Aeven

r

) = 0, 1, 0, 0, 1, 0, 0, 0, 1, . . . (so π2(BDiff∂(D4)) = 0)

4

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The theorem of Weiss

Closely related to the classical story is the fact that the stable map O = colim

d→∞ O(d) −

→ Top = colim

d→∞ Top(d)

is a Q-equivalence, and hence H∗(BTop; Q) ∼ = H∗(BO; Q) = Q[p1, p2, p3, . . .].

5

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The theorem of Weiss

Closely related to the classical story is the fact that the stable map O = colim

d→∞ O(d) −

→ Top = colim

d→∞ Top(d)

is a Q-equivalence, and hence H∗(BTop; Q) ∼ = H∗(BO; Q) = Q[p1, p2, p3, . . .]. In H∗(BO(2n); Q) the usual definition of Pontrjagin classes shows pn = e2 and pn+i = 0 for all i > 0. (!)

5

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The theorem of Weiss

Closely related to the classical story is the fact that the stable map O = colim

d→∞ O(d) −

→ Top = colim

d→∞ Top(d)

is a Q-equivalence, and hence H∗(BTop; Q) ∼ = H∗(BO; Q) = Q[p1, p2, p3, . . .]. In H∗(BO(2n); Q) the usual definition of Pontrjagin classes shows pn = e2 and pn+i = 0 for all i > 0. (!)

  • Theorem. [Weiss ’15]

For many n and i ≥ 0 there are classes wn,i ∈ π4(n+i)(BTop(2n)) which pair nontrivially with pn+i (i.e. (!) does not hold on BTop(2n)). ⇒ π2n−1+4i(BDiff∂(D2n)) ⊗ Q = 0 for such n and i.

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A pattern

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A pattern

Inspired by Weiss’ argument, Alexander Kupers and I have begun a programme to determine π∗(BDiff∂(D2n)) ⊗ Q as completely as possible. The first installment just came out:

  • A. Kupers, O. R-W, On diffeomorphisms of even-dimensional discs

(arXiv:2007.13884)

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A pattern

Inspired by Weiss’ argument, Alexander Kupers and I have begun a programme to determine π∗(BDiff∂(D2n)) ⊗ Q as completely as possible. The first installment just came out:

  • A. Kupers, O. R-W, On diffeomorphisms of even-dimensional discs

(arXiv:2007.13884)

Here we

  • 1. fully determine these groups in degrees ∗ ≤ 4n − 10,

6

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A pattern

Inspired by Weiss’ argument, Alexander Kupers and I have begun a programme to determine π∗(BDiff∂(D2n)) ⊗ Q as completely as possible. The first installment just came out:

  • A. Kupers, O. R-W, On diffeomorphisms of even-dimensional discs

(arXiv:2007.13884)

Here we

  • 1. fully determine these groups in degrees ∗ ≤ 4n − 10,
  • 2. determine them in higher degrees outside of certain “bands”,

6

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A pattern

Inspired by Weiss’ argument, Alexander Kupers and I have begun a programme to determine π∗(BDiff∂(D2n)) ⊗ Q as completely as possible. The first installment just came out:

  • A. Kupers, O. R-W, On diffeomorphisms of even-dimensional discs

(arXiv:2007.13884)

Here we

  • 1. fully determine these groups in degrees ∗ ≤ 4n − 10,
  • 2. determine them in higher degrees outside of certain “bands”,
  • 3. understand something about the structure of these bands.

6

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2 4 6 8 10 12 14 16 18 20 22 24 26 28 30 32 34 36 38 40 42 44 46 48 50 52 54 56 6 8 10 12 14 16 18 20 22 24 26 28 30 32 34 36 38 40 42 44 46 48 50 52 54 56 58 60 62 64

  • π∗(BDiff∂(D2n)) ⊗ Q

= Q{Weiss class} = uncertainty, but • survives = uncertainty, • may not survive 7

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A pattern

  • Theorem. [Kupers–R-W]

Let 2n ≥ 6. (i) If d < 2n − 1 then πd(BDiff ∂(D2n)) ⊗ Q vanishes, and (ii) if d ≥ 2n − 1 then πd(BDiff ∂(D2n)) ⊗ Q is            Q if d ≡ 2n−1 mod 4 and d / ∈

r≥2

[2r(n−2) − 1, 2rn − 1], if d ≡ 2n−1 mod 4 and d / ∈

r≥2

[2r(n−2) − 1, 2rn − 1], ?

  • therwise.

8

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A pattern

Using the fibre sequence Top(2n)

O(2n) → Top O(2n) → Top Top(2n) we have the

Reformulation (slightly stronger). For 2n ≥ 6 the groups π∗(Ω2n+1 (

Top Top(2n))) ⊗ Q are supported in

degrees ∗ ∈

  • r≥2

[2r(n − 2) − 1, 2rn − 2].

9

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A pattern

Using the fibre sequence Top(2n)

O(2n) → Top O(2n) → Top Top(2n) we have the

Reformulation (slightly stronger). For 2n ≥ 6 the groups π∗(Ω2n+1 (

Top Top(2n))) ⊗ Q are supported in

degrees ∗ ∈

  • r≥2

[2r(n − 2) − 1, 2rn − 2]. Reflecting D2n or R2n induces compatible involutions on Ω2n+1

Top Top(2n) −

→ BDiff ∂(D2n) ≃ Ω2n

Top(2n) O(2n) −

→ Ω2n

Top O(2n). 9

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A pattern

Using the fibre sequence Top(2n)

O(2n) → Top O(2n) → Top Top(2n) we have the

Reformulation (slightly stronger). For 2n ≥ 6 the groups π∗(Ω2n+1 (

Top Top(2n))) ⊗ Q are supported in

degrees ∗ ∈

  • r≥2

[2r(n − 2) − 1, 2rn − 2]. Reflecting D2n or R2n induces compatible involutions on Ω2n+1

Top Top(2n) −

→ BDiff ∂(D2n) ≃ Ω2n

Top(2n) O(2n) −

→ Ω2n

Top O(2n).

We show this acts as −1 on π∗(Ω2n

Top O(2n)) ⊗ Q = Q[2n − 1] ⊕ Q[2n + 3] ⊕ Q[2n + 7] ⊕ · · ·

and acts on π∗(Ω2n+1 (

Top Top(2n))) ⊗ Q as (−1)r in the rth band. 9

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A pattern

Using the fibre sequence Top(2n)

O(2n) → Top O(2n) → Top Top(2n) we have the

Reformulation (slightly stronger). For 2n ≥ 6 the groups π∗(Ω2n+1 (

Top Top(2n))) ⊗ Q are supported in

degrees ∗ ∈

  • r≥2

[2r(n − 2) − 1, 2rn − 2]. Reflecting D2n or R2n induces compatible involutions on Ω2n+1

Top Top(2n) −

→ BDiff ∂(D2n) ≃ Ω2n

Top(2n) O(2n) −

→ Ω2n

Top O(2n).

We show this acts as −1 on π∗(Ω2n

Top O(2n)) ⊗ Q = Q[2n − 1] ⊕ Q[2n + 3] ⊕ Q[2n + 7] ⊕ · · ·

and acts on π∗(Ω2n+1 (

Top Top(2n))) ⊗ Q as (−1)r in the rth band.

The orange/blue colours in the chart are the +1/−1 eigenspaces.

9

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The first uncertainty

We also determine to some extent what happens in the first band shown in the chart:

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The first uncertainty

We also determine to some extent what happens in the first band shown in the chart: the groups π∗(Ω2n+1(

Top Top(2n))) ⊗ Q in degrees

[4n − 9, 4n − 4] are calculated by a chain complex of the form Q2 Q4 Q10 Q21 Q15 Q3

10

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The first uncertainty

We also determine to some extent what happens in the first band shown in the chart: the groups π∗(Ω2n+1(

Top Top(2n))) ⊗ Q in degrees

[4n − 9, 4n − 4] are calculated by a chain complex of the form Q2 Q4 Q10 Q21 Q15 Q3 We don’t know the differentials, but it has Euler characteristic 1 so must have some homology. It lies in the +1-eigenspace, so injects into π∗(BDiff∂(D2n)) ⊗ Q.

10

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The first uncertainty

We also determine to some extent what happens in the first band shown in the chart: the groups π∗(Ω2n+1(

Top Top(2n))) ⊗ Q in degrees

[4n − 9, 4n − 4] are calculated by a chain complex of the form Q2 Q4 Q10 Q21 Q15 Q3 We don’t know the differentials, but it has Euler characteristic 1 so must have some homology. It lies in the +1-eigenspace, so injects into π∗(BDiff∂(D2n)) ⊗ Q. By analogy with Watanabe’s theorem for D4 one expects dim π4n−6(BDiff∂(D2n)) ⊗ Q ≥ 1 which is compatible with the above.

10

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Remarks on the proof

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Philosophy

Many results in this flavour of geometric topology are relative: they describe the difference between

  • 1. topological/smooth manifolds (smoothing)
  • 2. homotopy equivalences/block diffeomorphisms (surgery)
  • 3. block diffeomorphisms/diffeomorphisms (pseudoisotopy)

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Philosophy

Many results in this flavour of geometric topology are relative: they describe the difference between

  • 1. topological/smooth manifolds (smoothing)
  • 2. homotopy equivalences/block diffeomorphisms (surgery)
  • 3. block diffeomorphisms/diffeomorphisms (pseudoisotopy)

Weiss suggested a new kind of relativisation: for M with ∂M = Sd−1 and 1

2∂M := Dd−1 ⊂ Sd−1 he showed that

Diff∂(M) Diff∂(Dd) ≃ Emb

∼ = 1/2∂(M). 11

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Philosophy

Many results in this flavour of geometric topology are relative: they describe the difference between

  • 1. topological/smooth manifolds (smoothing)
  • 2. homotopy equivalences/block diffeomorphisms (surgery)
  • 3. block diffeomorphisms/diffeomorphisms (pseudoisotopy)

Weiss suggested a new kind of relativisation: for M with ∂M = Sd−1 and 1

2∂M := Dd−1 ⊂ Sd−1 he showed that

Diff∂(M) Diff∂(Dd) ≃ Emb

∼ = 1/2∂(M).

Under mild conditions on M such a self-embedding space can be analysed using the theory of embedding calculus. (The “codimension” of such embeddings can be ≥ 3.)

11

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Philosophy

Many results in this flavour of geometric topology are relative: they describe the difference between

  • 1. topological/smooth manifolds (smoothing)
  • 2. homotopy equivalences/block diffeomorphisms (surgery)
  • 3. block diffeomorphisms/diffeomorphisms (pseudoisotopy)

Weiss suggested a new kind of relativisation: for M with ∂M = Sd−1 and 1

2∂M := Dd−1 ⊂ Sd−1 he showed that

Diff∂(M) Diff∂(Dd) ≃ Emb

∼ = 1/2∂(M).

Under mild conditions on M such a self-embedding space can be analysed using the theory of embedding calculus. (The “codimension” of such embeddings can be ≥ 3.) Strategy: find a manifold M for which one can understand Emb

∼ = 1/2∂(M) and Diff∂(M), then deduce things about Diff∂(Dd). 11

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The manifold Wg,1

A good choice is Wg,1 := D2n#g(Sn × Sn) especially for “arbitrarily large” g.

12

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The manifold Wg,1

A good choice is Wg,1 := D2n#g(Sn × Sn) especially for “arbitrarily large” g.

  • Theorem. [Madsen–Weiss ’07 2n = 2, Galatius–R-W ’14 2n ≥ 4]

lim

g→∞ H∗(BDiff∂(Wg,1); Q) = Q[κc | c ∈ B]

Here B is the set of monomials in e, pn−1, pn−2, . . . , p⌈ n+1

4 ⌉. 12

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SLIDE 48

The manifold Wg,1

A good choice is Wg,1 := D2n#g(Sn × Sn) especially for “arbitrarily large” g.

  • Theorem. [Madsen–Weiss ’07 2n = 2, Galatius–R-W ’14 2n ≥ 4]

lim

g→∞ H∗(BDiff∂(Wg,1); Q) = Q[κc | c ∈ B]

Here B is the set of monomials in e, pn−1, pn−2, . . . , p⌈ n+1

4 ⌉.

  • Theorem. [Berglund–Madsen ’20 2n ≥ 6]

lim

g→∞ H∗(B

Diff ∂(Wg,1); Q) = Q[˜ κξ

c | (c, ξ) ∈ B′]

lim

g→∞ H∗(BhAut∂(Wg,1); Q) = Q[˜

κξ

c | (c, ξ) ∈ B′′]

Here B′ and B′′ are much more complicated than B, and we will probably never be able to enumerate them completely.

12

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Difficulties I

Embedding calculus describes Emb

∼ = 1/2∂(Wg,1) as the limit of a tower

T1Emb

∼ = 1/2∂(Wg,1)

T2Emb

∼ = 1/2∂(Wg,1)

T3Emb

∼ = 1/2∂(Wg,1) · · ·

L2Emb

∼ = 1/2∂(Wg,1)

L3Emb

∼ = 1/2∂(Wg,1) 13

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SLIDE 50

Difficulties I

Embedding calculus describes Emb

∼ = 1/2∂(Wg,1) as the limit of a tower

T1Emb

∼ = 1/2∂(Wg,1)

T2Emb

∼ = 1/2∂(Wg,1)

T3Emb

∼ = 1/2∂(Wg,1) · · ·

L2Emb

∼ = 1/2∂(Wg,1)

L3Emb

∼ = 1/2∂(Wg,1)

The term T1Emb

∼ = 1/2∂(Wg,1) is close to being the space of homotopy

self-equivalences of Wg,1 relative to half the boundary; if we instead use framed self-embeddings then it is: T1Emb

∼ =,fr 1/2∂(Wg,1) ≃ hAut ∼ = 1/2∂(Wg,1)

(and the higher layers don’t change).

13

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SLIDE 51

Difficulties I

Embedding calculus describes Emb

∼ = 1/2∂(Wg,1) as the limit of a tower

T1Emb

∼ = 1/2∂(Wg,1)

T2Emb

∼ = 1/2∂(Wg,1)

T3Emb

∼ = 1/2∂(Wg,1) · · ·

L2Emb

∼ = 1/2∂(Wg,1)

L3Emb

∼ = 1/2∂(Wg,1)

The term T1Emb

∼ = 1/2∂(Wg,1) is close to being the space of homotopy

self-equivalences of Wg,1 relative to half the boundary; if we instead use framed self-embeddings then it is: T1Emb

∼ =,fr 1/2∂(Wg,1) ≃ hAut ∼ = 1/2∂(Wg,1)

(and the higher layers don’t change). By rational homotopy theory, for L := Lie(s−1Hn(Wg,1; Q)) have π∗>0(hAut1/2∂(Wg,1)) ⊗ Q = Der+(L, L) = HomQ(s−1Hn(Wg,1; Q), L), supported in degrees which are multiples of n − 1.

13

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Difficulties I

The higher layers are described as spaces of sections LkEmb

∼ = 1/2∂(Wg,1) ≃ Γ∂

      Zk tohofibI⊆[k]Emb(I, Wg,1) Confk(Wg,1)      

14

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Difficulties I

The higher layers are described as spaces of sections LkEmb

∼ = 1/2∂(Wg,1) ≃ Γ∂

      Zk tohofibI⊆[k]Emb(I, Wg,1) Confk(Wg,1)       The homotopy groups of such a space can be computed by a twisted form of the Federer spectral sequence. Rationally express this as E2

p,q ⊗ Q = [Hp(Wk g,1, ∆1/2∂; Q) ⊗ πq(tohofibI⊆[k]Emb(I, Wg,1))]Sk

⇒ πq−p(LkEmb

∼ = 1/2∂(Wg,1)) ⊗ Q. 14

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SLIDE 54

Difficulties I

The higher layers are described as spaces of sections LkEmb

∼ = 1/2∂(Wg,1) ≃ Γ∂

      Zk tohofibI⊆[k]Emb(I, Wg,1) Confk(Wg,1)       The homotopy groups of such a space can be computed by a twisted form of the Federer spectral sequence. Rationally express this as E2

p,q ⊗ Q = [Hp(Wk g,1, ∆1/2∂; Q) ⊗ πq(tohofibI⊆[k]Emb(I, Wg,1))]Sk

⇒ πq−p(LkEmb

∼ = 1/2∂(Wg,1)) ⊗ Q.

The main issue is to determine/estimate the characters of Hp(Wk

g,1, ∆1/2∂; Q)

and πq(Emb([k], Wg,1)) ⊗ Q as representations of Sk × π0(Diff∂(Wg,1)).

14

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SLIDE 55

Difficulties I

The character of Hp(Wk

g,1, ∆1/2∂; Q) can be determined easily using a

theorem of Petersen ’20. The character of πq(Emb([k], Wg,1)) ⊗ Q is much more complicated.

15

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SLIDE 56

Difficulties I

The character of Hp(Wk

g,1, ∆1/2∂; Q) can be determined easily using a

theorem of Petersen ’20. The character of πq(Emb([k], Wg,1)) ⊗ Q is much more complicated. Briefly: identify these homotopy groups with an extended form of the Drinfel’d–Kohno Lie algebra; show that up to filtration this is Koszul, and identify its Koszul dual with the Kriz–Totaro algebra; show that the collection of all Kriz–Totaro algebras for all k may be given a new—external—product, and that they form a free commutative algebra with this product; calculate.

15

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SLIDE 57

Difficulties I

The character of Hp(Wk

g,1, ∆1/2∂; Q) can be determined easily using a

theorem of Petersen ’20. The character of πq(Emb([k], Wg,1)) ⊗ Q is much more complicated. Briefly: identify these homotopy groups with an extended form of the Drinfel’d–Kohno Lie algebra; show that up to filtration this is Koszul, and identify its Koszul dual with the Kriz–Totaro algebra; show that the collection of all Kriz–Totaro algebras for all k may be given a new—external—product, and that they form a free commutative algebra with this product; calculate. We are able to completely determine rational homotopy of the layers of the embedding calculus tower, but not their interaction.

15

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SLIDE 58

Difficulties I

The character of Hp(Wk

g,1, ∆1/2∂; Q) can be determined easily using a

theorem of Petersen ’20. The character of πq(Emb([k], Wg,1)) ⊗ Q is much more complicated. Briefly: identify these homotopy groups with an extended form of the Drinfel’d–Kohno Lie algebra; show that up to filtration this is Koszul, and identify its Koszul dual with the Kriz–Totaro algebra; show that the collection of all Kriz–Totaro algebras for all k may be given a new—external—product, and that they form a free commutative algebra with this product; calculate. We are able to completely determine rational homotopy of the layers of the embedding calculus tower, but not their interaction. Nonetheless this lets us prove that π∗(Emb

∼ =,fr 1/2∂(Wg,1))⊗Q

is supported in degrees ∗ ∈ ∪r≥1[r(n − 2) − 1, r(n − 1)]. This is the darkly shaded region in the chart.

15

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SLIDE 59

Difficulties II

While we have very good understanding of H∗(BDiff∂(Wg,1); Q), the strategy requires π∗(BDiff∂(Wg,1)) ⊗ Q.

16

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SLIDE 60

Difficulties II

While we have very good understanding of H∗(BDiff∂(Wg,1); Q), the strategy requires π∗(BDiff∂(Wg,1)) ⊗ Q. π1(BDiff∂(Wg,1)) ∼ Sp2g(Z) (n odd) or Og,g(Z) (n even) ⇒ wildly complicated group, not nilpotent: cannot expect to determine the rational homotopy of BDiff∂(Wg,1) from cohomology.

16

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SLIDE 61

Difficulties II

While we have very good understanding of H∗(BDiff∂(Wg,1); Q), the strategy requires π∗(BDiff∂(Wg,1)) ⊗ Q. π1(BDiff∂(Wg,1)) ∼ Sp2g(Z) (n odd) or Og,g(Z) (n even) ⇒ wildly complicated group, not nilpotent: cannot expect to determine the rational homotopy of BDiff∂(Wg,1) from cohomology. Can pass to the Torelli subgroup Tor∂(Wg,1) := ker(Diff∂(Wg,1) → Aut(Hn(Wg,1; Z))) to eliminate the arithmetic group, but this changes the cohomology.

16

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SLIDE 62

Difficulties II

While we have very good understanding of H∗(BDiff∂(Wg,1); Q), the strategy requires π∗(BDiff∂(Wg,1)) ⊗ Q. π1(BDiff∂(Wg,1)) ∼ Sp2g(Z) (n odd) or Og,g(Z) (n even) ⇒ wildly complicated group, not nilpotent: cannot expect to determine the rational homotopy of BDiff∂(Wg,1) from cohomology. Can pass to the Torelli subgroup Tor∂(Wg,1) := ker(Diff∂(Wg,1) → Aut(Hn(Wg,1; Z))) to eliminate the arithmetic group, but this changes the cohomology. In two companion papers we prove that the space BTor∂(Wg,1) is nilpotent, and determine H∗(BTor∂(Wg,1); Q) as g → ∞.

  • A. Kupers, O. R-W, On the cohomology of Torelli groups

Forum of Mathematics, Pi, 8 (2020)

  • A. Kupers, O. R-W, The cohomology of Torelli groups is algebraic

Forum of Mathematics, Sigma, to appear

16

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SLIDE 63

Difficulties II

Adapting this to the framed case, we produce a fibration X1(g) − → BTorfr

∂ (Wg,1) −

→ X0 with H∗(X0; Q) = Q[¯ σ4j−2n−1 | j > n/2].

17

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SLIDE 64

Difficulties II

Adapting this to the framed case, we produce a fibration X1(g) − → BTorfr

∂ (Wg,1) −

→ X0 with H∗(X0; Q) = Q[¯ σ4j−2n−1 | j > n/2]. We show that in a stable range, H∗(X1(g); Q) is generated by classes κ(v1 ⊗ · · · ⊗ vr) ∈ H(r−2)n(X1(g); Q) r ≥ 3, vi ∈ Hn(Wg,1; Q) subject only to the relations (where {ai} and {a#

i } are dual bases)

(i) linearity in each vi, (ii) κ(vσ(1) ⊗ vσ(2) ⊗ · · · ⊗ vσ(r)) = sign(σ)n · κ(v1 ⊗ v2 ⊗ · · · ⊗ vr), (iii)

i κ(v ⊗ ai) · κ(a# i ⊗ w) = κ(v ⊗ w), for any tensors v and w,

(iv)

i κ(v ⊗ ai ⊗ a# i ) = 0 for any tensor v. 17

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SLIDE 65

Difficulties II

Adapting this to the framed case, we produce a fibration X1(g) − → BTorfr

∂ (Wg,1) −

→ X0 with H∗(X0; Q) = Q[¯ σ4j−2n−1 | j > n/2]. We show that in a stable range, H∗(X1(g); Q) is generated by classes κ(v1 ⊗ · · · ⊗ vr) ∈ H(r−2)n(X1(g); Q) r ≥ 3, vi ∈ Hn(Wg,1; Q) subject only to the relations (where {ai} and {a#

i } are dual bases)

(i) linearity in each vi, (ii) κ(vσ(1) ⊗ vσ(2) ⊗ · · · ⊗ vσ(r)) = sign(σ)n · κ(v1 ⊗ v2 ⊗ · · · ⊗ vr), (iii)

i κ(v ⊗ ai) · κ(a# i ⊗ w) = κ(v ⊗ w), for any tensors v and w,

(iv)

i κ(v ⊗ ai ⊗ a# i ) = 0 for any tensor v.

The unstable Adams spectral sequence then shows π∗(BTorfr

∂ (Wg,1))⊗Q =

 

j>n/2

Q[4j − 2n − 1]   “⊕”

  • something supported in

∗∈

r≥0[r(n−1)+1,rn−2]

  • The second piece is the lightly shaded region in the chart.

17

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SLIDE 66

Optimism

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SLIDE 67

Divergent embedding calculus

Can apply embedding calculus to diffeomorphisms, considered as codimension 0 embeddings. It need not converge and in fact does not converge: by work of Fresse, Turchin, and Willwacher ’17 it predicts (modulo a subtlety) that π∗(BDiff∂(D2n)) ⊗ Q should be

  • i>0

Q[2n − 4i]

  • ⊕ Q[4n − 6] ⊕ Q[8n − 10] ⊕ Q[10n − 15] ⊕ · · ·

so misses the Weiss classes and starts with some spurious classes. But apart from this it has classes supported in our bands, and here is given precisely by Kontsevich’s graph complex GC2

2n. 18

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SLIDE 68

Divergent embedding calculus

Can apply embedding calculus to diffeomorphisms, considered as codimension 0 embeddings. It need not converge and in fact does not converge: by work of Fresse, Turchin, and Willwacher ’17 it predicts (modulo a subtlety) that π∗(BDiff∂(D2n)) ⊗ Q should be

  • i>0

Q[2n − 4i]

  • ⊕ Q[4n − 6] ⊕ Q[8n − 10] ⊕ Q[10n − 15] ⊕ · · ·

so misses the Weiss classes and starts with some spurious classes. But apart from this it has classes supported in our bands, and here is given precisely by Kontsevich’s graph complex GC2

2n.

Could there be a rational fibration BDiff∂(D2n) − → BT∞Diff∂(D2n) − → Ω∞+2nL(Z)?

18

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SLIDE 69

Evidence

Could there be a rational fibration BDiff∂(D2n) − → BT∞Diff∂(D2n) − → Ω∞+2nL(Z)? Evidence. It is consistent with everything we know, and would explain Watanabe’s and Weiss’ results.

19

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SLIDE 70

Evidence

Could there be a rational fibration BDiff∂(D2n) − → BT∞Diff∂(D2n) − → Ω∞+2nL(Z)? Evidence. It is consistent with everything we know, and would explain Watanabe’s and Weiss’ results.

  • Evidence. [Knudsen–Kupers ’20]

If d ≥ 6, Md 2-connected, ∂M = Sd−1 then hofib(BDiff∂(M) → BT∞Diff∂(M)) is independent of M.

19

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SLIDE 71

Evidence

Could there be a rational fibration BDiff∂(D2n) − → BT∞Diff∂(D2n) − → Ω∞+2nL(Z)? Evidence. It is consistent with everything we know, and would explain Watanabe’s and Weiss’ results.

  • Evidence. [Knudsen–Kupers ’20]

If d ≥ 6, Md 2-connected, ∂M = Sd−1 then hofib(BDiff∂(M) → BT∞Diff∂(M)) is independent of M.

  • Evidence. [Prigge ’20]

The family signature theorem does not hold on BT2Diff∂(M).

19

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SLIDE 72

Questions?

19

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SLIDE 73

2 4 6 8 10 12 14 16 18 20 22 24 26 28 30 32 34 36 38 40 42 44 46 48 50 52 54 56 6 8 10 12 14 16 18 20 22 24 26 28 30 32 34 36 38 40 42 44 46 48 50 52 54 56 58 60 62 64

  • π∗(BDiff∂(D2n)) ⊗ Q

= Q{Weiss class} = uncertainty, but • survives = uncertainty, • may not survive 20