Towards an understanding of ramified extensions of structured ring - - PowerPoint PPT Presentation

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Towards an understanding of ramified extensions of structured ring - - PowerPoint PPT Presentation

Towards an understanding of ramified extensions of structured ring spectra Birgit Richter Joint work with Bjrn Dundas, Ayelet Lindenstrauss Women in Homotopy Theory and Algebraic Geometry Structured ring spectra Slogan: Nice cohomology


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Towards an understanding of ramified extensions

  • f structured ring spectra

Birgit Richter Joint work with Bjørn Dundas, Ayelet Lindenstrauss Women in Homotopy Theory and Algebraic Geometry

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Structured ring spectra

Slogan: Nice cohomology theories behave like commutative rings.

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Structured ring spectra

Slogan: Nice cohomology theories behave like commutative rings. Brown: Cohomology theories can be represented by spectra: E n(X) ∼ = [X, En]

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Structured ring spectra

Slogan: Nice cohomology theories behave like commutative rings. Brown: Cohomology theories can be represented by spectra: E n(X) ∼ = [X, En] (En): family of spaces with En ≃ ΩEn+1.

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Structured ring spectra

Slogan: Nice cohomology theories behave like commutative rings. Brown: Cohomology theories can be represented by spectra: E n(X) ∼ = [X, En] (En): family of spaces with En ≃ ΩEn+1. Since the mid 90’s: There are (several) symmetric monoidal model categories whose homotopy categories are Quillen equivalent to the good old stable homotopy category:

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Structured ring spectra

Slogan: Nice cohomology theories behave like commutative rings. Brown: Cohomology theories can be represented by spectra: E n(X) ∼ = [X, En] (En): family of spaces with En ≃ ΩEn+1. Since the mid 90’s: There are (several) symmetric monoidal model categories whose homotopy categories are Quillen equivalent to the good old stable homotopy category:

◮ Symmetric spectra (Hovey, Shipley, Smith)

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Structured ring spectra

Slogan: Nice cohomology theories behave like commutative rings. Brown: Cohomology theories can be represented by spectra: E n(X) ∼ = [X, En] (En): family of spaces with En ≃ ΩEn+1. Since the mid 90’s: There are (several) symmetric monoidal model categories whose homotopy categories are Quillen equivalent to the good old stable homotopy category:

◮ Symmetric spectra (Hovey, Shipley, Smith) ◮ S-modules (Elmendorf-Kriz-Mandell-May aka EKMM)

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Structured ring spectra

Slogan: Nice cohomology theories behave like commutative rings. Brown: Cohomology theories can be represented by spectra: E n(X) ∼ = [X, En] (En): family of spaces with En ≃ ΩEn+1. Since the mid 90’s: There are (several) symmetric monoidal model categories whose homotopy categories are Quillen equivalent to the good old stable homotopy category:

◮ Symmetric spectra (Hovey, Shipley, Smith) ◮ S-modules (Elmendorf-Kriz-Mandell-May aka EKMM) ◮ ...

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Structured ring spectra

Slogan: Nice cohomology theories behave like commutative rings. Brown: Cohomology theories can be represented by spectra: E n(X) ∼ = [X, En] (En): family of spaces with En ≃ ΩEn+1. Since the mid 90’s: There are (several) symmetric monoidal model categories whose homotopy categories are Quillen equivalent to the good old stable homotopy category:

◮ Symmetric spectra (Hovey, Shipley, Smith) ◮ S-modules (Elmendorf-Kriz-Mandell-May aka EKMM) ◮ ...

We are interested in commutative monoids (commutative ring spectra) and their algebraic properties.

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Examples

You all know examples of such commutative ring spectra:

◮ Take your favorite commutative ring R and consider singular

cohomology with coefficients in R, H∗(−; R). The representing spectrum is the Eilenberg-MacLane spectrum of R, HR.

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Examples

You all know examples of such commutative ring spectra:

◮ Take your favorite commutative ring R and consider singular

cohomology with coefficients in R, H∗(−; R). The representing spectrum is the Eilenberg-MacLane spectrum of R, HR. The multiplication in R turns HR into a commutative ring spectrum.

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Examples

You all know examples of such commutative ring spectra:

◮ Take your favorite commutative ring R and consider singular

cohomology with coefficients in R, H∗(−; R). The representing spectrum is the Eilenberg-MacLane spectrum of R, HR. The multiplication in R turns HR into a commutative ring spectrum.

◮ Topological complex K-theory, KU0(X), measures how many

different complex vector bundles of finite rank live over your space X.

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Examples

You all know examples of such commutative ring spectra:

◮ Take your favorite commutative ring R and consider singular

cohomology with coefficients in R, H∗(−; R). The representing spectrum is the Eilenberg-MacLane spectrum of R, HR. The multiplication in R turns HR into a commutative ring spectrum.

◮ Topological complex K-theory, KU0(X), measures how many

different complex vector bundles of finite rank live over your space X. You consider isomorphism classes of complex vector bundles of finite rank over X, VectC(X). This is an abelian monoid wrt the Whitney sum of vector bundles.

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Examples

You all know examples of such commutative ring spectra:

◮ Take your favorite commutative ring R and consider singular

cohomology with coefficients in R, H∗(−; R). The representing spectrum is the Eilenberg-MacLane spectrum of R, HR. The multiplication in R turns HR into a commutative ring spectrum.

◮ Topological complex K-theory, KU0(X), measures how many

different complex vector bundles of finite rank live over your space X. You consider isomorphism classes of complex vector bundles of finite rank over X, VectC(X). This is an abelian monoid wrt the Whitney sum of vector bundles. Then group completion gives KU0(X): KU0(X) = Gr(VectC(X)).

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This can be extended to a cohomology theory KU∗(−) with representing spectrum KU. The tensor product of vector bundles gives KU the structure of a commutative ring spectrum.

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This can be extended to a cohomology theory KU∗(−) with representing spectrum KU. The tensor product of vector bundles gives KU the structure of a commutative ring spectrum.

◮ Topological real K-theory, KO0(X), is defined similarly, using

real instead of complex vector bundles.

◮ Stable cohomotopy is represented by the sphere spectrum S.

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This can be extended to a cohomology theory KU∗(−) with representing spectrum KU. The tensor product of vector bundles gives KU the structure of a commutative ring spectrum.

◮ Topological real K-theory, KO0(X), is defined similarly, using

real instead of complex vector bundles.

◮ Stable cohomotopy is represented by the sphere spectrum S.

Spectra have stable homotopy groups:

◮ π∗(HR) = H−∗(pt; R) = R concentrated in degree zero.

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This can be extended to a cohomology theory KU∗(−) with representing spectrum KU. The tensor product of vector bundles gives KU the structure of a commutative ring spectrum.

◮ Topological real K-theory, KO0(X), is defined similarly, using

real instead of complex vector bundles.

◮ Stable cohomotopy is represented by the sphere spectrum S.

Spectra have stable homotopy groups:

◮ π∗(HR) = H−∗(pt; R) = R concentrated in degree zero. ◮ π∗(KU) = Z[u±1], with |u| = 2. The class u is the Bott class.

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This can be extended to a cohomology theory KU∗(−) with representing spectrum KU. The tensor product of vector bundles gives KU the structure of a commutative ring spectrum.

◮ Topological real K-theory, KO0(X), is defined similarly, using

real instead of complex vector bundles.

◮ Stable cohomotopy is represented by the sphere spectrum S.

Spectra have stable homotopy groups:

◮ π∗(HR) = H−∗(pt; R) = R concentrated in degree zero. ◮ π∗(KU) = Z[u±1], with |u| = 2. The class u is the Bott class. ◮ The homotopy groups of KO are more complicated.

π∗(KO) = Z[η, y, w±1]/2η, η3, ηy, y2−4w, |η| = 1, |w| = 8.

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This can be extended to a cohomology theory KU∗(−) with representing spectrum KU. The tensor product of vector bundles gives KU the structure of a commutative ring spectrum.

◮ Topological real K-theory, KO0(X), is defined similarly, using

real instead of complex vector bundles.

◮ Stable cohomotopy is represented by the sphere spectrum S.

Spectra have stable homotopy groups:

◮ π∗(HR) = H−∗(pt; R) = R concentrated in degree zero. ◮ π∗(KU) = Z[u±1], with |u| = 2. The class u is the Bott class. ◮ The homotopy groups of KO are more complicated.

π∗(KO) = Z[η, y, w±1]/2η, η3, ηy, y2−4w, |η| = 1, |w| = 8. The map that assigns to a real vector bundle its complexified vector bundle induces a ring map c : KO → KU. Its effect on homotopy groups is η → 0, y → 2u2, w → u4. In particular, π∗(KU) is a graded commutative π∗(KO)-algebra.

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Galois extensions of structured ring spectra

Actually, KU is a commutative KO-algebra spectrum.

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Galois extensions of structured ring spectra

Actually, KU is a commutative KO-algebra spectrum. Complex conjugation gives rise to a C2-action on KU with homotopy fixed points KO.

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Galois extensions of structured ring spectra

Actually, KU is a commutative KO-algebra spectrum. Complex conjugation gives rise to a C2-action on KU with homotopy fixed points KO. In a suitable sense KU is unramified over KO: KU ∧KO KU ≃ KU × KU.

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Galois extensions of structured ring spectra

Actually, KU is a commutative KO-algebra spectrum. Complex conjugation gives rise to a C2-action on KU with homotopy fixed points KO. In a suitable sense KU is unramified over KO: KU ∧KO KU ≃ KU × KU. Rognes ’08: KU is a C2-Galois extension of KO.

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Galois extensions of structured ring spectra

Actually, KU is a commutative KO-algebra spectrum. Complex conjugation gives rise to a C2-action on KU with homotopy fixed points KO. In a suitable sense KU is unramified over KO: KU ∧KO KU ≃ KU × KU. Rognes ’08: KU is a C2-Galois extension of KO. Definition (Rognes ’08) (up to cofibrancy issues..., G finite) A commutative A-algebra spectrum B is a G-Galois extension, if G acts on B via maps of commutative A-algebras

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Galois extensions of structured ring spectra

Actually, KU is a commutative KO-algebra spectrum. Complex conjugation gives rise to a C2-action on KU with homotopy fixed points KO. In a suitable sense KU is unramified over KO: KU ∧KO KU ≃ KU × KU. Rognes ’08: KU is a C2-Galois extension of KO. Definition (Rognes ’08) (up to cofibrancy issues..., G finite) A commutative A-algebra spectrum B is a G-Galois extension, if G acts on B via maps of commutative A-algebras such that the maps

◮ i : A → BhG and

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Galois extensions of structured ring spectra

Actually, KU is a commutative KO-algebra spectrum. Complex conjugation gives rise to a C2-action on KU with homotopy fixed points KO. In a suitable sense KU is unramified over KO: KU ∧KO KU ≃ KU × KU. Rognes ’08: KU is a C2-Galois extension of KO. Definition (Rognes ’08) (up to cofibrancy issues..., G finite) A commutative A-algebra spectrum B is a G-Galois extension, if G acts on B via maps of commutative A-algebras such that the maps

◮ i : A → BhG and ◮ h: B ∧A B → G B

(∗) are weak equivalences.

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Galois extensions of structured ring spectra

Actually, KU is a commutative KO-algebra spectrum. Complex conjugation gives rise to a C2-action on KU with homotopy fixed points KO. In a suitable sense KU is unramified over KO: KU ∧KO KU ≃ KU × KU. Rognes ’08: KU is a C2-Galois extension of KO. Definition (Rognes ’08) (up to cofibrancy issues..., G finite) A commutative A-algebra spectrum B is a G-Galois extension, if G acts on B via maps of commutative A-algebras such that the maps

◮ i : A → BhG and ◮ h: B ∧A B → G B

(∗) are weak equivalences. This definition is a direct generalization of the definition of Galois extensions of commutative rings (due to Auslander-Goldman).

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Examples

As a sanity check we have:

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Examples

As a sanity check we have: Rognes ’08: Let R → T be a map of commutative rings and let G act on T via R-algebra maps. Then R → T is a G-Galois extension of commutative rings iff HR → HT is a G-Galois extension of commutative ring spectra.

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Examples

As a sanity check we have: Rognes ’08: Let R → T be a map of commutative rings and let G act on T via R-algebra maps. Then R → T is a G-Galois extension of commutative rings iff HR → HT is a G-Galois extension of commutative ring spectra. Let Q ⊂ K be a finite G-Galois extension of fields and let OK denote the ring of integers in K. Then Z → OK is never unramified, hence HZ → HOK is never a G-Galois extension.

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Examples

As a sanity check we have: Rognes ’08: Let R → T be a map of commutative rings and let G act on T via R-algebra maps. Then R → T is a G-Galois extension of commutative rings iff HR → HT is a G-Galois extension of commutative ring spectra. Let Q ⊂ K be a finite G-Galois extension of fields and let OK denote the ring of integers in K. Then Z → OK is never unramified, hence HZ → HOK is never a G-Galois extension. Z → Z[i] is wildly ramified at 2, hence Z[i] ⊗Z Z[i] is not isomorphic to Z[i] × Z[i].

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Examples

As a sanity check we have: Rognes ’08: Let R → T be a map of commutative rings and let G act on T via R-algebra maps. Then R → T is a G-Galois extension of commutative rings iff HR → HT is a G-Galois extension of commutative ring spectra. Let Q ⊂ K be a finite G-Galois extension of fields and let OK denote the ring of integers in K. Then Z → OK is never unramified, hence HZ → HOK is never a G-Galois extension. Z → Z[i] is wildly ramified at 2, hence Z[i] ⊗Z Z[i] is not isomorphic to Z[i] × Z[i]. Z[ 1

2] → Z[i, 1 2], however, is C2-Galois.

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Examples, continued

We saw KO → KU already.

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Examples, continued

We saw KO → KU already. Take an odd prime p. Then KU(p) splits as KU(p) ≃

p−2

  • i=0

Σ2iL.

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Examples, continued

We saw KO → KU already. Take an odd prime p. Then KU(p) splits as KU(p) ≃

p−2

  • i=0

Σ2iL. L is called the Adams summand of KU.

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Examples, continued

We saw KO → KU already. Take an odd prime p. Then KU(p) splits as KU(p) ≃

p−2

  • i=0

Σ2iL. L is called the Adams summand of KU. Rognes ’08: Lp → KUp is a Cp−1-Galois extension. Here, the Cp−1-action is generated by an Adams operation.

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Connective covers

If we want to understand arithmetic properties of a commutative ring spectrum R, then we try to understand its algebraic K-theory, K(R).

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Connective covers

If we want to understand arithmetic properties of a commutative ring spectrum R, then we try to understand its algebraic K-theory, K(R). K(R) is hard to compute. It can be approximated by easier things like topological Hochschild homology (THH(R)) or topological cyclic homology (TC(R)).

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Connective covers

If we want to understand arithmetic properties of a commutative ring spectrum R, then we try to understand its algebraic K-theory, K(R). K(R) is hard to compute. It can be approximated by easier things like topological Hochschild homology (THH(R)) or topological cyclic homology (TC(R)). There are trace maps K(R)

trc tr

  • TC(R)
  • THH(R)
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Connective covers

If we want to understand arithmetic properties of a commutative ring spectrum R, then we try to understand its algebraic K-theory, K(R). K(R) is hard to compute. It can be approximated by easier things like topological Hochschild homology (THH(R)) or topological cyclic homology (TC(R)). There are trace maps K(R)

trc tr

  • TC(R)
  • THH(R)

BUT: Trace methods work for connective spectra, these are spectra with trivial negative homotopy groups.

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Connective spectra

For any commutative ring spectrum R, there is a commutative ring spectrum r with a map j : r → R such that π∗(j) is an isomorphism for all ∗ ≥ 0.

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Connective spectra

For any commutative ring spectrum R, there is a commutative ring spectrum r with a map j : r → R such that π∗(j) is an isomorphism for all ∗ ≥ 0. For instance, we get ko

c

  • j
  • ku

j

  • KO

c

KU

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Connective spectra

For any commutative ring spectrum R, there is a commutative ring spectrum r with a map j : r → R such that π∗(j) is an isomorphism for all ∗ ≥ 0. For instance, we get ko

c

  • j
  • ku

j

  • KO

c

KU

BUT: A theorem of Akhil Mathew tells us, that if A → B is G-Galois for finite G and A and B are connective, then π∗(A) → π∗(B) is ´ etale.

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Connective spectra

For any commutative ring spectrum R, there is a commutative ring spectrum r with a map j : r → R such that π∗(j) is an isomorphism for all ∗ ≥ 0. For instance, we get ko

c

  • j
  • ku

j

  • KO

c

KU

BUT: A theorem of Akhil Mathew tells us, that if A → B is G-Galois for finite G and A and B are connective, then π∗(A) → π∗(B) is ´ etale. π∗(ko) = Z[η, y, w]/2η, η3, ηy, y2 − 4w. → π∗(ku) = Z[u] is certainly not ´ etale.

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Connective spectra

For any commutative ring spectrum R, there is a commutative ring spectrum r with a map j : r → R such that π∗(j) is an isomorphism for all ∗ ≥ 0. For instance, we get ko

c

  • j
  • ku

j

  • KO

c

KU

BUT: A theorem of Akhil Mathew tells us, that if A → B is G-Galois for finite G and A and B are connective, then π∗(A) → π∗(B) is ´ etale. π∗(ko) = Z[η, y, w]/2η, η3, ηy, y2 − 4w. → π∗(ku) = Z[u] is certainly not ´ etale. We have to live with ramification!

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Wild ramification

c : ko → ku fails in two aspects:

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Wild ramification

c : ko → ku fails in two aspects:

◮ ko is not equivalent to kuhC2 (but closely related to...)

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Wild ramification

c : ko → ku fails in two aspects:

◮ ko is not equivalent to kuhC2 (but closely related to...) ◮ h: ku ∧ko ku → C2 ku is not a weak equivalence

(but ku ∧ko ku ≃ ku ∨ Σ2ku).

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Wild ramification

c : ko → ku fails in two aspects:

◮ ko is not equivalent to kuhC2 (but closely related to...) ◮ h: ku ∧ko ku → C2 ku is not a weak equivalence

(but ku ∧ko ku ≃ ku ∨ Σ2ku). Theorem (Dundas, Lindenstrauss, R) ko → ku is wildly ramified.

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Wild ramification

c : ko → ku fails in two aspects:

◮ ko is not equivalent to kuhC2 (but closely related to...) ◮ h: ku ∧ko ku → C2 ku is not a weak equivalence

(but ku ∧ko ku ≃ ku ∨ Σ2ku). Theorem (Dundas, Lindenstrauss, R) ko → ku is wildly ramified. How do we measure ramification?

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Relative THH

If we have a G-action on a commutative A-algebra B and if h: B ∧A B →

G B is a weak equivalence, then Rognes shows

that the canonical map B → THHA(B) is a weak equivalence.

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Relative THH

If we have a G-action on a commutative A-algebra B and if h: B ∧A B →

G B is a weak equivalence, then Rognes shows

that the canonical map B → THHA(B) is a weak equivalence. What is THHA(B)?

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Relative THH

If we have a G-action on a commutative A-algebra B and if h: B ∧A B →

G B is a weak equivalence, then Rognes shows

that the canonical map B → THHA(B) is a weak equivalence. What is THHA(B)? Topological Hochschild homology of B as an A-algebra, i.e.,

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Relative THH

If we have a G-action on a commutative A-algebra B and if h: B ∧A B →

G B is a weak equivalence, then Rognes shows

that the canonical map B → THHA(B) is a weak equivalence. What is THHA(B)? Topological Hochschild homology of B as an A-algebra, i.e., THHA(B) is the geometric realization of the simplicial spectrum · · ·

  • B ∧A B ∧A B
  • B ∧A B
  • B
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THHA(B) measure the ramification of A → B!

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THHA(B) measure the ramification of A → B! If B is commutative, then we get maps B → THHA(B) → B whose composite is the identity on B.

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THHA(B) measure the ramification of A → B! If B is commutative, then we get maps B → THHA(B) → B whose composite is the identity on B. Thus B splits off THHA(B). If THHA(B) is larger than B, then A → B is ramified.

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THHA(B) measure the ramification of A → B! If B is commutative, then we get maps B → THHA(B) → B whose composite is the identity on B. Thus B splits off THHA(B). If THHA(B) is larger than B, then A → B is ramified. We abbreviate π∗(THHA(B)) with THHA

∗ (B).

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The ko → ku-case

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The ko → ku-case

Theorem (DLR)

◮ As a graded commutative augmented π∗(ku)-algebra

π∗(ku ∧ko ku) ∼ = π∗(ku)[˜ u]/˜ u2 − u2 with |˜ u| = 2.

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The ko → ku-case

Theorem (DLR)

◮ As a graded commutative augmented π∗(ku)-algebra

π∗(ku ∧ko ku) ∼ = π∗(ku)[˜ u]/˜ u2 − u2 with |˜ u| = 2.

◮ The Tor spectral sequence

E 2

∗,∗ = Torπ∗(ku∧koku) ∗,∗

(π∗(ku), π∗(ku)) ⇒ THHko

∗ (ku)

collapses at the E 2-page.

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The ko → ku-case

Theorem (DLR)

◮ As a graded commutative augmented π∗(ku)-algebra

π∗(ku ∧ko ku) ∼ = π∗(ku)[˜ u]/˜ u2 − u2 with |˜ u| = 2.

◮ The Tor spectral sequence

E 2

∗,∗ = Torπ∗(ku∧koku) ∗,∗

(π∗(ku), π∗(ku)) ⇒ THHko

∗ (ku)

collapses at the E 2-page.

◮ THHko ∗ (ku) is a square zero extension of π∗(ku):

THHko

∗ (ku) ∼

= π∗(ku) ⋊ π∗(ku)/2uy0, y1, . . . with |yj| = (1 + |u|)(2j + 1) = 3(2j + 1).

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Comparison to Z → Z[i]

The result is very similar to the calculation of HH∗(Z[i]) = THHHZ(HZ[i]) (Larsen-Lindenstrauss):

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Comparison to Z → Z[i]

The result is very similar to the calculation of HH∗(Z[i]) = THHHZ(HZ[i]) (Larsen-Lindenstrauss): HHZ

∗ (Z[i]) ∼

= THHHZ

(HZ[i]) =      Z[i], for ∗ = 0, Z[i]/2i, for odd ∗, 0,

  • therwise.
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Comparison to Z → Z[i]

The result is very similar to the calculation of HH∗(Z[i]) = THHHZ(HZ[i]) (Larsen-Lindenstrauss): HHZ

∗ (Z[i]) ∼

= THHHZ

(HZ[i]) =      Z[i], for ∗ = 0, Z[i]/2i, for odd ∗, 0,

  • therwise.

Hence HHZ

∗ (Z[i]) ∼

= Z[i] ⋊ (Z[i]/2i)yj, j ≥ 0 with |yj| = 2j + 1.

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SLIDE 67

Idea of proof for ko → ku:

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SLIDE 68

Idea of proof for ko → ku: Use an explicit resolution to get that the E 2-page is the homology

  • f

. . .

0 Σ4π∗(ku) 2u Σ2π∗(ku)

π∗(ku).

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SLIDE 69

Idea of proof for ko → ku: Use an explicit resolution to get that the E 2-page is the homology

  • f

. . .

0 Σ4π∗(ku) 2u Σ2π∗(ku)

π∗(ku).

As π∗(ku) splits off THHko

∗ (ku) the zero column has to survive and

cannot be hit by differentials and hence all differentials are trivial.

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SLIDE 70

Idea of proof for ko → ku: Use an explicit resolution to get that the E 2-page is the homology

  • f

. . .

0 Σ4π∗(ku) 2u Σ2π∗(ku)

π∗(ku).

As π∗(ku) splits off THHko

∗ (ku) the zero column has to survive and

cannot be hit by differentials and hence all differentials are trivial. Use that the spectral sequence is one of π∗(ku)-modules to rule

  • ut additive extensions.
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SLIDE 71

Idea of proof for ko → ku: Use an explicit resolution to get that the E 2-page is the homology

  • f

. . .

0 Σ4π∗(ku) 2u Σ2π∗(ku)

π∗(ku).

As π∗(ku) splits off THHko

∗ (ku) the zero column has to survive and

cannot be hit by differentials and hence all differentials are trivial. Use that the spectral sequence is one of π∗(ku)-modules to rule

  • ut additive extensions.

Since the generators over π∗(ku) are all in odd degree, and their products cannot hit the direct summand π∗(ku) in filtration degree zero, their products are all zero.

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SLIDE 72

Contrast to tame ramification

Consider and odd prime p and ℓ

  • j
  • ku(p)

j

  • L

KU(p)

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SLIDE 73

Contrast to tame ramification

Consider and odd prime p and ℓ

  • j
  • ku(p)

j

  • L

KU(p)

π∗(ℓ) = Z(p)[v1] → Z(p)[u] = π∗(ku(p)), v1 → up−1 already looks much nicer.

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SLIDE 74

Contrast to tame ramification

Consider and odd prime p and ℓ

  • j
  • ku(p)

j

  • L

KU(p)

π∗(ℓ) = Z(p)[v1] → Z(p)[u] = π∗(ku(p)), v1 → up−1 already looks much nicer.

◮ Rognes: ku(p) → THHℓ(ku(p)) is a K(1)-local equivalence.

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SLIDE 75

Contrast to tame ramification

Consider and odd prime p and ℓ

  • j
  • ku(p)

j

  • L

KU(p)

π∗(ℓ) = Z(p)[v1] → Z(p)[u] = π∗(ku(p)), v1 → up−1 already looks much nicer.

◮ Rognes: ku(p) → THHℓ(ku(p)) is a K(1)-local equivalence. ◮ Sagave: The map ℓ → ku(p) is log-´

etale.

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SLIDE 76

Contrast to tame ramification

Consider and odd prime p and ℓ

  • j
  • ku(p)

j

  • L

KU(p)

π∗(ℓ) = Z(p)[v1] → Z(p)[u] = π∗(ku(p)), v1 → up−1 already looks much nicer.

◮ Rognes: ku(p) → THHℓ(ku(p)) is a K(1)-local equivalence. ◮ Sagave: The map ℓ → ku(p) is log-´

etale.

◮ Ausoni proved that the p-completed extension even satisfies

Galois descent for THH and algebraic K-theory: THH(kup)hCp−1 ≃ THH(ℓp), K(kup)hCp−1 ≃ K(ℓp).

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SLIDE 77

Tame ramification is visible!

ℓ → ku(p) behaves like a tamely ramified extension:

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SLIDE 78

Tame ramification is visible!

ℓ → ku(p) behaves like a tamely ramified extension: Theorem (DLR) THHℓ

∗(ku(p)) ∼

= π∗(ku(p))∗ ⋊ π∗(ku(p))y0, y1, . . ./up−2 where the degree of yi is 2pi + 3.

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SLIDE 79

Tame ramification is visible!

ℓ → ku(p) behaves like a tamely ramified extension: Theorem (DLR) THHℓ

∗(ku(p)) ∼

= π∗(ku(p))∗ ⋊ π∗(ku(p))y0, y1, . . ./up−2 where the degree of yi is 2pi + 3. p − 1 is a p-local unit, hence no additive integral torsion appears in THHℓ

∗(ku(p)).

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SLIDE 80

Other important examples

There are ring spectra E(n), called Johnson-Wilson spectra.

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SLIDE 81

Other important examples

There are ring spectra E(n), called Johnson-Wilson spectra. π∗(E(n)) = Z(p)[v1, . . . , vn−1, v±1

n ], |vi| = 2pi − 2.

slide-82
SLIDE 82

Other important examples

There are ring spectra E(n), called Johnson-Wilson spectra. π∗(E(n)) = Z(p)[v1, . . . , vn−1, v±1

n ], |vi| = 2pi − 2.

These are synthetic spectra: For almost all n and p there is no geometric interpretation for E(n).

slide-83
SLIDE 83

Other important examples

There are ring spectra E(n), called Johnson-Wilson spectra. π∗(E(n)) = Z(p)[v1, . . . , vn−1, v±1

n ], |vi| = 2pi − 2.

These are synthetic spectra: For almost all n and p there is no geometric interpretation for E(n). Exceptions: At an odd prime: E(1) = L,

slide-84
SLIDE 84

Other important examples

There are ring spectra E(n), called Johnson-Wilson spectra. π∗(E(n)) = Z(p)[v1, . . . , vn−1, v±1

n ], |vi| = 2pi − 2.

These are synthetic spectra: For almost all n and p there is no geometric interpretation for E(n). Exceptions: At an odd prime: E(1) = L, E(2) at 2 can be constructed out of tmf1(3)(2) by inverting a3. (Similar: E(2) at 3, using a Shimura curve)

slide-85
SLIDE 85

Other important examples

There are ring spectra E(n), called Johnson-Wilson spectra. π∗(E(n)) = Z(p)[v1, . . . , vn−1, v±1

n ], |vi| = 2pi − 2.

These are synthetic spectra: For almost all n and p there is no geometric interpretation for E(n). Exceptions: At an odd prime: E(1) = L, E(2) at 2 can be constructed out of tmf1(3)(2) by inverting a3. (Similar: E(2) at 3, using a Shimura curve) All the E(n) for n ≥ 1 carry a C2-action that comes from complex conjugation on complex bordism.

slide-86
SLIDE 86

Other important examples

There are ring spectra E(n), called Johnson-Wilson spectra. π∗(E(n)) = Z(p)[v1, . . . , vn−1, v±1

n ], |vi| = 2pi − 2.

These are synthetic spectra: For almost all n and p there is no geometric interpretation for E(n). Exceptions: At an odd prime: E(1) = L, E(2) at 2 can be constructed out of tmf1(3)(2) by inverting a3. (Similar: E(2) at 3, using a Shimura curve) All the E(n) for n ≥ 1 carry a C2-action that comes from complex conjugation on complex bordism. Are the E(n)hC2 → E(n) C2-Galois extensions?

slide-87
SLIDE 87

Other important examples

There are ring spectra E(n), called Johnson-Wilson spectra. π∗(E(n)) = Z(p)[v1, . . . , vn−1, v±1

n ], |vi| = 2pi − 2.

These are synthetic spectra: For almost all n and p there is no geometric interpretation for E(n). Exceptions: At an odd prime: E(1) = L, E(2) at 2 can be constructed out of tmf1(3)(2) by inverting a3. (Similar: E(2) at 3, using a Shimura curve) All the E(n) for n ≥ 1 carry a C2-action that comes from complex conjugation on complex bordism. Are the E(n)hC2 → E(n) C2-Galois extensions? Yes, for n = 1, p = 2. That’s the example KO(2) → KU(2).

slide-88
SLIDE 88

Other important examples

There are ring spectra E(n), called Johnson-Wilson spectra. π∗(E(n)) = Z(p)[v1, . . . , vn−1, v±1

n ], |vi| = 2pi − 2.

These are synthetic spectra: For almost all n and p there is no geometric interpretation for E(n). Exceptions: At an odd prime: E(1) = L, E(2) at 2 can be constructed out of tmf1(3)(2) by inverting a3. (Similar: E(2) at 3, using a Shimura curve) All the E(n) for n ≥ 1 carry a C2-action that comes from complex conjugation on complex bordism. Are the E(n)hC2 → E(n) C2-Galois extensions? Yes, for n = 1, p = 2. That’s the example KO(2) → KU(2). Tmf0(3) → Tmf1(3) is C2-Galois (Mathew, Meier) and closely related to E(2)hC2 → E(2).

slide-89
SLIDE 89

Other important examples

There are ring spectra E(n), called Johnson-Wilson spectra. π∗(E(n)) = Z(p)[v1, . . . , vn−1, v±1

n ], |vi| = 2pi − 2.

These are synthetic spectra: For almost all n and p there is no geometric interpretation for E(n). Exceptions: At an odd prime: E(1) = L, E(2) at 2 can be constructed out of tmf1(3)(2) by inverting a3. (Similar: E(2) at 3, using a Shimura curve) All the E(n) for n ≥ 1 carry a C2-action that comes from complex conjugation on complex bordism. Are the E(n)hC2 → E(n) C2-Galois extensions? Yes, for n = 1, p = 2. That’s the example KO(2) → KU(2). Tmf0(3) → Tmf1(3) is C2-Galois (Mathew, Meier) and closely related to E(2)hC2 → E(2). We can control certain quotient maps, e.g. tmf1(3)(2) → ku(2).

slide-90
SLIDE 90

Open questions

◮ Problem: We do not know whether the E(n) are commutative

ring spectra for all n and p. (Motivic help?)

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SLIDE 91

Open questions

◮ Problem: We do not know whether the E(n) are commutative

ring spectra for all n and p. (Motivic help?)

◮ Is there more variation than just tame and wild ramification?

slide-92
SLIDE 92

Open questions

◮ Problem: We do not know whether the E(n) are commutative

ring spectra for all n and p. (Motivic help?)

◮ Is there more variation than just tame and wild ramification? ◮ Can there be ramification at chromatic primes rather than

integral primes?

slide-93
SLIDE 93

Open questions

◮ Problem: We do not know whether the E(n) are commutative

ring spectra for all n and p. (Motivic help?)

◮ Is there more variation than just tame and wild ramification? ◮ Can there be ramification at chromatic primes rather than

integral primes?

◮ How bad is tmf0(3) → tmf1(3)?

slide-94
SLIDE 94

Open questions

◮ Problem: We do not know whether the E(n) are commutative

ring spectra for all n and p. (Motivic help?)

◮ Is there more variation than just tame and wild ramification? ◮ Can there be ramification at chromatic primes rather than

integral primes?

◮ How bad is tmf0(3) → tmf1(3)? ◮ Can we understand the ramification for the extentions

BPnhC2 → BPn for higher n? Here, π∗(BPn) = Z(p)[v1, . . . , vn].

slide-95
SLIDE 95

Open questions

◮ Problem: We do not know whether the E(n) are commutative

ring spectra for all n and p. (Motivic help?)

◮ Is there more variation than just tame and wild ramification? ◮ Can there be ramification at chromatic primes rather than

integral primes?

◮ How bad is tmf0(3) → tmf1(3)? ◮ Can we understand the ramification for the extentions

BPnhC2 → BPn for higher n? Here, π∗(BPn) = Z(p)[v1, . . . , vn]. BP2 has commutative models at p = 2, 3 (Hill, Lawson, Naumann)

◮ Are ku, ko and ℓ analogues of rings of integers in their

periodic versions, i.e., ku = OKU, ko = OKO, ℓ = OL?

slide-96
SLIDE 96

Open questions

◮ Problem: We do not know whether the E(n) are commutative

ring spectra for all n and p. (Motivic help?)

◮ Is there more variation than just tame and wild ramification? ◮ Can there be ramification at chromatic primes rather than

integral primes?

◮ How bad is tmf0(3) → tmf1(3)? ◮ Can we understand the ramification for the extentions

BPnhC2 → BPn for higher n? Here, π∗(BPn) = Z(p)[v1, . . . , vn]. BP2 has commutative models at p = 2, 3 (Hill, Lawson, Naumann)

◮ Are ku, ko and ℓ analogues of rings of integers in their

periodic versions, i.e., ku = OKU, ko = OKO, ℓ = OL? What is a good notion of OK for periodic ring spectra K?

slide-97
SLIDE 97

Open questions

◮ Problem: We do not know whether the E(n) are commutative

ring spectra for all n and p. (Motivic help?)

◮ Is there more variation than just tame and wild ramification? ◮ Can there be ramification at chromatic primes rather than

integral primes?

◮ How bad is tmf0(3) → tmf1(3)? ◮ Can we understand the ramification for the extentions

BPnhC2 → BPn for higher n? Here, π∗(BPn) = Z(p)[v1, . . . , vn]. BP2 has commutative models at p = 2, 3 (Hill, Lawson, Naumann)

◮ Are ku, ko and ℓ analogues of rings of integers in their

periodic versions, i.e., ku = OKU, ko = OKO, ℓ = OL? What is a good notion of OK for periodic ring spectra K?

◮ ???