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Relative p -adic Hodge theory Kiran S. Kedlaya Department of - - PowerPoint PPT Presentation

Relative p -adic Hodge theory Kiran S. Kedlaya Department of Mathematics, University of California, San Diego kedlaya@ucsd.edu http://kskedlaya.org/slides/ Hot Topics: Perfectoid Spaces and their Applications MSRI, Berkeley, February 19, 2014


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SLIDE 1

Relative p-adic Hodge theory

Kiran S. Kedlaya

Department of Mathematics, University of California, San Diego kedlaya@ucsd.edu http://kskedlaya.org/slides/

Hot Topics: Perfectoid Spaces and their Applications MSRI, Berkeley, February 19, 2014 Joint work with Ruochuan Liu (BICMR, Beijing): Relative p-adic Hodge theory, I: Foundations, arXiv:1301.0792v2 (2014). Relative p-adic Hodge theory, II: Imperfect period rings (in revision).

Supported by NSF (grant DMS-1101343), UCSD (Warschawski chair). Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 1 / 36

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Contents

1

Overview: goals of relative p-adic Hodge theory

2

Period sheaves I: Witt vectors and Zp-local systems

3

Period sheaves II: Robba rings and Qp-local systems

4

Sheaves on relative Fargues-Fontaine curves

5

The next frontier: imperfect period rings (and maybe sheaves)

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 2 / 36

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SLIDE 3

Overview: goals of relative p-adic Hodge theory

Contents

1

Overview: goals of relative p-adic Hodge theory

2

Period sheaves I: Witt vectors and Zp-local systems

3

Period sheaves II: Robba rings and Qp-local systems

4

Sheaves on relative Fargues-Fontaine curves

5

The next frontier: imperfect period rings (and maybe sheaves)

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 3 / 36

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SLIDE 4

Overview: goals of relative p-adic Hodge theory

Disclaimer

The term “p-adic Hodge theory” encompasses two aspects: external p-adic Hodge theory: comparison of cohomology theorems (´ etale, de Rham, crystalline, etc.) for algebraic varieties over p-adic fields; or internal p-adic Hodge theory: analysis of continuous p-adic representations of Galois groups of p-adic fields, including but not limited to ´ etale cohomology of algebraic varieties. In this talk, only the internal theory is considered. For the external theory in a similar relative setting, see Nizio l’s lectures.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 4 / 36

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SLIDE 5

Overview: goals of relative p-adic Hodge theory

Disclaimer

The term “p-adic Hodge theory” encompasses two aspects: external p-adic Hodge theory: comparison of cohomology theorems (´ etale, de Rham, crystalline, etc.) for algebraic varieties over p-adic fields; or internal p-adic Hodge theory: analysis of continuous p-adic representations of Galois groups of p-adic fields, including but not limited to ´ etale cohomology of algebraic varieties. In this talk, only the internal theory is considered. For the external theory in a similar relative setting, see Nizio l’s lectures.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 4 / 36

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SLIDE 6

Overview: goals of relative p-adic Hodge theory

Disclaimer

The term “p-adic Hodge theory” encompasses two aspects: external p-adic Hodge theory: comparison of cohomology theorems (´ etale, de Rham, crystalline, etc.) for algebraic varieties over p-adic fields; or internal p-adic Hodge theory: analysis of continuous p-adic representations of Galois groups of p-adic fields, including but not limited to ´ etale cohomology of algebraic varieties. In this talk, only the internal theory is considered. For the external theory in a similar relative setting, see Nizio l’s lectures.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 4 / 36

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SLIDE 7

Overview: goals of relative p-adic Hodge theory

Disclaimer

The term “p-adic Hodge theory” encompasses two aspects: external p-adic Hodge theory: comparison of cohomology theorems (´ etale, de Rham, crystalline, etc.) for algebraic varieties over p-adic fields; or internal p-adic Hodge theory: analysis of continuous p-adic representations of Galois groups of p-adic fields, including but not limited to ´ etale cohomology of algebraic varieties. In this talk, only the internal theory is considered. For the external theory in a similar relative setting, see Nizio l’s lectures.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 4 / 36

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SLIDE 8

Overview: goals of relative p-adic Hodge theory

Galois representations

Let K be a p-adic field (a field of characteristic 0 complete for a discrete valuation whose residue field is perfect of characteristic p) with absolute Galois group GK. In p-adic Hodge theory, one studies the categories RepZp(GK) and RepQp(GK) of continuous representations of GK on finitely generated Zp-modules and Qp-modules. Note that the latter is the isogeny category

  • f the former; that is, every Qp-representation admits GK-stable lattices.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 5 / 36

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SLIDE 9

Overview: goals of relative p-adic Hodge theory

Galois representations

Let K be a p-adic field (a field of characteristic 0 complete for a discrete valuation whose residue field is perfect of characteristic p) with absolute Galois group GK. In p-adic Hodge theory, one studies the categories RepZp(GK) and RepQp(GK) of continuous representations of GK on finitely generated Zp-modules and Qp-modules. Note that the latter is the isogeny category

  • f the former; that is, every Qp-representation admits GK-stable lattices.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 5 / 36

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SLIDE 10

Overview: goals of relative p-adic Hodge theory

Local systems on analytic spaces

Let X be an adic space locally of finite type over K. For ∗ ∈ {Zp, Qp}, by an ´ etale ∗-local system on X, we will mean a sheaf on Xpro´

et which is

pro-´ etale locally of the form V : Y → Mapcont(|Y | , V ) (“constant sheaf”) for V a finitely generated ∗-module with its usual topology. For instance, if X = Spa(K, K ◦) this is just an object of Rep∗(GK): take the neighborhood Y = Spa(CK, C◦

K).

In general, ´ etale Qp-local systems are not simply Zp-local systems up to isogeny! There are many natural examples arising from ´ etale covers with noncompact groups of deck transformations: Tate uniformization of elliptic curves, Drinfel’d uniformizations, Rapaport-Zink period morphisms...

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 6 / 36

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SLIDE 11

Overview: goals of relative p-adic Hodge theory

Local systems on analytic spaces

Let X be an adic space locally of finite type over K. For ∗ ∈ {Zp, Qp}, by an ´ etale ∗-local system on X, we will mean a sheaf on Xpro´

et which is

pro-´ etale locally of the form V : Y → Mapcont(|Y | , V ) (“constant sheaf”) for V a finitely generated ∗-module with its usual topology. For instance, if X = Spa(K, K ◦) this is just an object of Rep∗(GK): take the neighborhood Y = Spa(CK, C◦

K).

In general, ´ etale Qp-local systems are not simply Zp-local systems up to isogeny! There are many natural examples arising from ´ etale covers with noncompact groups of deck transformations: Tate uniformization of elliptic curves, Drinfel’d uniformizations, Rapaport-Zink period morphisms...

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 6 / 36

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SLIDE 12

Overview: goals of relative p-adic Hodge theory

Local systems via perfectoid spaces

For K a p-adic field, one studies RepQp(GK) by passing from K to some sufficiently ramified (strictly arithmetically profinite) algebraic extension K∞ of K. Then K∞ is perfectoid; by tilting (and Krasner’s lemma) RepQp(GK∞) ∼ = RepQp(G

K∞) ∼

= RepQp(G

K∞

♭)

so we can use the Frobenius on K∞

♭ to study this category.

To study RepQp(GK), one must add descent data; often one takes K∞/K Galois with Γ = Gal(K∞/K) a p-adic Lie group (e.g., K∞ = K(µp∞) with Γ ⊆ Z×

p ), and the descent data becomes a Γ-action.

But descent data can also be viewed as a sheaf condition for the pro-´ etale topology, in which case we can consider all choices for K∞ at once! This point of view adapts well to analytic spaces, using perfectoid algebras as the analogue of strictly APF extensions.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 7 / 36

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SLIDE 13

Overview: goals of relative p-adic Hodge theory

Local systems via perfectoid spaces

For K a p-adic field, one studies RepQp(GK) by passing from K to some sufficiently ramified (strictly arithmetically profinite) algebraic extension K∞ of K. Then K∞ is perfectoid; by tilting (and Krasner’s lemma) RepQp(GK∞) ∼ = RepQp(G

K∞) ∼

= RepQp(G

K∞

♭)

so we can use the Frobenius on K∞

♭ to study this category.

To study RepQp(GK), one must add descent data; often one takes K∞/K Galois with Γ = Gal(K∞/K) a p-adic Lie group (e.g., K∞ = K(µp∞) with Γ ⊆ Z×

p ), and the descent data becomes a Γ-action.

But descent data can also be viewed as a sheaf condition for the pro-´ etale topology, in which case we can consider all choices for K∞ at once! This point of view adapts well to analytic spaces, using perfectoid algebras as the analogue of strictly APF extensions.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 7 / 36

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SLIDE 14

Overview: goals of relative p-adic Hodge theory

Local systems via perfectoid spaces

For K a p-adic field, one studies RepQp(GK) by passing from K to some sufficiently ramified (strictly arithmetically profinite) algebraic extension K∞ of K. Then K∞ is perfectoid; by tilting (and Krasner’s lemma) RepQp(GK∞) ∼ = RepQp(G

K∞) ∼

= RepQp(G

K∞

♭)

so we can use the Frobenius on K∞

♭ to study this category.

To study RepQp(GK), one must add descent data; often one takes K∞/K Galois with Γ = Gal(K∞/K) a p-adic Lie group (e.g., K∞ = K(µp∞) with Γ ⊆ Z×

p ), and the descent data becomes a Γ-action.

But descent data can also be viewed as a sheaf condition for the pro-´ etale topology, in which case we can consider all choices for K∞ at once! This point of view adapts well to analytic spaces, using perfectoid algebras as the analogue of strictly APF extensions.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 7 / 36

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SLIDE 15

Period sheaves I: Witt vectors and Zp-local systems

Contents

1

Overview: goals of relative p-adic Hodge theory

2

Period sheaves I: Witt vectors and Zp-local systems

3

Period sheaves II: Robba rings and Qp-local systems

4

Sheaves on relative Fargues-Fontaine curves

5

The next frontier: imperfect period rings (and maybe sheaves)

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 8 / 36

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SLIDE 16

Period sheaves I: Witt vectors and Zp-local systems

A simplifying assumption

Hereafter, X is an adic space over Qp which is uniform: it is locally Spa(A, A+) where A is a Banach algebra over Qp whose norm is submultiplicative (|xy| ≤ |x||y|) and power-multiplicative (|x2| = |x|2). In particular X is reduced. This restriction is harmless for our purposes: Any perfectoid space is uniform. For any adic space X over Qp, there is a unique closed immersed subspace X u of X which is uniform and satisfies |X u| = |X|, X u

´ et ∼

= X´

et, and X u pro´ et ∼

= Xpro´

et.

Any adic space coming from a reduced rigid analytic space or a reduced Berkovich strictly1 analytic space has this property. Our constructions generally do not see A+; this is related to the fact that Spa(A, A◦) → Spa(A, A+) retracts onto its subspace of rank 1 valuations.

1Berkovich’s non-strictly analytic spaces do not correspond to adic spaces; one needs

a parallel adic theory where elements of value groups are always comparable with R.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 9 / 36

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SLIDE 17

Period sheaves I: Witt vectors and Zp-local systems

A simplifying assumption

Hereafter, X is an adic space over Qp which is uniform: it is locally Spa(A, A+) where A is a Banach algebra over Qp whose norm is submultiplicative (|xy| ≤ |x||y|) and power-multiplicative (|x2| = |x|2). In particular X is reduced. This restriction is harmless for our purposes: Any perfectoid space is uniform. For any adic space X over Qp, there is a unique closed immersed subspace X u of X which is uniform and satisfies |X u| = |X|, X u

´ et ∼

= X´

et, and X u pro´ et ∼

= Xpro´

et.

Any adic space coming from a reduced rigid analytic space or a reduced Berkovich strictly1 analytic space has this property. Our constructions generally do not see A+; this is related to the fact that Spa(A, A◦) → Spa(A, A+) retracts onto its subspace of rank 1 valuations.

1Berkovich’s non-strictly analytic spaces do not correspond to adic spaces; one needs

a parallel adic theory where elements of value groups are always comparable with R.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 9 / 36

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SLIDE 18

Period sheaves I: Witt vectors and Zp-local systems

A simplifying assumption

Hereafter, X is an adic space over Qp which is uniform: it is locally Spa(A, A+) where A is a Banach algebra over Qp whose norm is submultiplicative (|xy| ≤ |x||y|) and power-multiplicative (|x2| = |x|2). In particular X is reduced. This restriction is harmless for our purposes: Any perfectoid space is uniform. For any adic space X over Qp, there is a unique closed immersed subspace X u of X which is uniform and satisfies |X u| = |X|, X u

´ et ∼

= X´

et, and X u pro´ et ∼

= Xpro´

et.

Any adic space coming from a reduced rigid analytic space or a reduced Berkovich strictly1 analytic space has this property. Our constructions generally do not see A+; this is related to the fact that Spa(A, A◦) → Spa(A, A+) retracts onto its subspace of rank 1 valuations.

1Berkovich’s non-strictly analytic spaces do not correspond to adic spaces; one needs

a parallel adic theory where elements of value groups are always comparable with R.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 9 / 36

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SLIDE 19

Period sheaves I: Witt vectors and Zp-local systems

A simplifying assumption

Hereafter, X is an adic space over Qp which is uniform: it is locally Spa(A, A+) where A is a Banach algebra over Qp whose norm is submultiplicative (|xy| ≤ |x||y|) and power-multiplicative (|x2| = |x|2). In particular X is reduced. This restriction is harmless for our purposes: Any perfectoid space is uniform. For any adic space X over Qp, there is a unique closed immersed subspace X u of X which is uniform and satisfies |X u| = |X|, X u

´ et ∼

= X´

et, and X u pro´ et ∼

= Xpro´

et.

Any adic space coming from a reduced rigid analytic space or a reduced Berkovich strictly1 analytic space has this property. Our constructions generally do not see A+; this is related to the fact that Spa(A, A◦) → Spa(A, A+) retracts onto its subspace of rank 1 valuations.

1Berkovich’s non-strictly analytic spaces do not correspond to adic spaces; one needs

a parallel adic theory where elements of value groups are always comparable with R.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 9 / 36

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SLIDE 20

Period sheaves I: Witt vectors and Zp-local systems

A simplifying assumption

Hereafter, X is an adic space over Qp which is uniform: it is locally Spa(A, A+) where A is a Banach algebra over Qp whose norm is submultiplicative (|xy| ≤ |x||y|) and power-multiplicative (|x2| = |x|2). In particular X is reduced. This restriction is harmless for our purposes: Any perfectoid space is uniform. For any adic space X over Qp, there is a unique closed immersed subspace X u of X which is uniform and satisfies |X u| = |X|, X u

´ et ∼

= X´

et, and X u pro´ et ∼

= Xpro´

et.

Any adic space coming from a reduced rigid analytic space or a reduced Berkovich strictly1 analytic space has this property. Our constructions generally do not see A+; this is related to the fact that Spa(A, A◦) → Spa(A, A+) retracts onto its subspace of rank 1 valuations.

1Berkovich’s non-strictly analytic spaces do not correspond to adic spaces; one needs

a parallel adic theory where elements of value groups are always comparable with R.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 9 / 36

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SLIDE 21

Period sheaves I: Witt vectors and Zp-local systems

Affinoid perfectoid subspaces

For this section, let’s assume2 that X is locally (strongly) noetherian. Then we may associate to X its pro-´ etale topology Xpro´

et as in de Jong’s lecture.

For Y = (Yi) ∈ Xpro´

et, the structure sheaf on Xpro´ et is

OX : Y → lim − →

i

O(Yi). Each term in this limit inherits a power-multiplicative norm, its spectral

  • norm. This norm is also the supremum over the valuations in Yi,

normalized p-adically. Recall from de Jong’s lecture that Xpro´

et has a neighborhood basis

consisting of affinoid perfectoid subspaces (i.e., each Yi comes from an adic ring and the completed inverse limit of these is perfectoid).

2This excludes X perfectoid, but it might be helpful to pretend that this is allowed. Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 10 / 36

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SLIDE 22

Period sheaves I: Witt vectors and Zp-local systems

Affinoid perfectoid subspaces

For this section, let’s assume2 that X is locally (strongly) noetherian. Then we may associate to X its pro-´ etale topology Xpro´

et as in de Jong’s lecture.

For Y = (Yi) ∈ Xpro´

et, the structure sheaf on Xpro´ et is

OX : Y → lim − →

i

O(Yi). Each term in this limit inherits a power-multiplicative norm, its spectral

  • norm. This norm is also the supremum over the valuations in Yi,

normalized p-adically. Recall from de Jong’s lecture that Xpro´

et has a neighborhood basis

consisting of affinoid perfectoid subspaces (i.e., each Yi comes from an adic ring and the completed inverse limit of these is perfectoid).

2This excludes X perfectoid, but it might be helpful to pretend that this is allowed. Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 10 / 36

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SLIDE 23

Period sheaves I: Witt vectors and Zp-local systems

Affinoid perfectoid subspaces

For this section, let’s assume2 that X is locally (strongly) noetherian. Then we may associate to X its pro-´ etale topology Xpro´

et as in de Jong’s lecture.

For Y = (Yi) ∈ Xpro´

et, the structure sheaf on Xpro´ et is

OX : Y → lim − →

i

O(Yi). Each term in this limit inherits a power-multiplicative norm, its spectral

  • norm. This norm is also the supremum over the valuations in Yi,

normalized p-adically. Recall from de Jong’s lecture that Xpro´

et has a neighborhood basis

consisting of affinoid perfectoid subspaces (i.e., each Yi comes from an adic ring and the completed inverse limit of these is perfectoid).

2This excludes X perfectoid, but it might be helpful to pretend that this is allowed. Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 10 / 36

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SLIDE 24

Period sheaves I: Witt vectors and Zp-local systems

The completed structure sheaf

From now on, let Y denote an arbitrary affinoid perfectoid in Xpro´

  • et. We

will specify a number of additional sheaves on Xpro´

et in terms of their

values on Y ; no promises are made about values on other pro-´ etale opens. Proposition-Definition There is a sheaf OX on Xpro´

et such that

OX(Y ) is the completion of O(Y ) for the spectral norm. Proposition-Definition There is a sheaf OX on Xpro´

et such that OX(Y ) =

O(Y )♭.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 11 / 36

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SLIDE 25

Period sheaves I: Witt vectors and Zp-local systems

The completed structure sheaf

From now on, let Y denote an arbitrary affinoid perfectoid in Xpro´

  • et. We

will specify a number of additional sheaves on Xpro´

et in terms of their

values on Y ; no promises are made about values on other pro-´ etale opens. Proposition-Definition There is a sheaf OX on Xpro´

et such that

OX(Y ) is the completion of O(Y ) for the spectral norm. Proposition-Definition There is a sheaf OX on Xpro´

et such that OX(Y ) =

O(Y )♭.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 11 / 36

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SLIDE 26

Period sheaves I: Witt vectors and Zp-local systems

The completed structure sheaf

From now on, let Y denote an arbitrary affinoid perfectoid in Xpro´

  • et. We

will specify a number of additional sheaves on Xpro´

et in terms of their

values on Y ; no promises are made about values on other pro-´ etale opens. Proposition-Definition There is a sheaf OX on Xpro´

et such that

OX(Y ) is the completion of O(Y ) for the spectral norm. Proposition-Definition There is a sheaf OX on Xpro´

et such that OX(Y ) =

O(Y )♭.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 11 / 36

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SLIDE 27

Period sheaves I: Witt vectors and Zp-local systems

Sheaves of (overconvergent) Witt vectors

For R a perfect ring of characteristic p, the ring W (R) of Witt vectors is p-adically separated and complete and W (R)/(p) = R. Reduction modulo p admits a multiplicative section, the Teichm¨ uller map x → [x]. Proposition-Definition There is a sheaf ˜ AX on Xpro´

et such that ˜

AX(Y ) = W (OX(Y )). Proposition-Definition If R carries a power-multiplicative norm, then for r > 0, the set W r(R) of x = ∞

n=0 pn[xn] ∈ W (R) with limn→∞ pn|xn|r = 0 is a subring of W (R).

Proposition-Definition For any r > 0, there is a sheaf ˜ A†,r

X on Xpro´ et such that

˜ A†,r

X (Y ) = W r(OX(Y )). Put ˜

A†

X = lim

− →r→0+ ˜ A†,r

X .

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 12 / 36

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SLIDE 28

Period sheaves I: Witt vectors and Zp-local systems

Sheaves of (overconvergent) Witt vectors

For R a perfect ring of characteristic p, the ring W (R) of Witt vectors is p-adically separated and complete and W (R)/(p) = R. Reduction modulo p admits a multiplicative section, the Teichm¨ uller map x → [x]. Proposition-Definition There is a sheaf ˜ AX on Xpro´

et such that ˜

AX(Y ) = W (OX(Y )). Proposition-Definition If R carries a power-multiplicative norm, then for r > 0, the set W r(R) of x = ∞

n=0 pn[xn] ∈ W (R) with limn→∞ pn|xn|r = 0 is a subring of W (R).

Proposition-Definition For any r > 0, there is a sheaf ˜ A†,r

X on Xpro´ et such that

˜ A†,r

X (Y ) = W r(OX(Y )). Put ˜

A†

X = lim

− →r→0+ ˜ A†,r

X .

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 12 / 36

slide-29
SLIDE 29

Period sheaves I: Witt vectors and Zp-local systems

Sheaves of (overconvergent) Witt vectors

For R a perfect ring of characteristic p, the ring W (R) of Witt vectors is p-adically separated and complete and W (R)/(p) = R. Reduction modulo p admits a multiplicative section, the Teichm¨ uller map x → [x]. Proposition-Definition There is a sheaf ˜ AX on Xpro´

et such that ˜

AX(Y ) = W (OX(Y )). Proposition-Definition If R carries a power-multiplicative norm, then for r > 0, the set W r(R) of x = ∞

n=0 pn[xn] ∈ W (R) with limn→∞ pn|xn|r = 0 is a subring of W (R).

Proposition-Definition For any r > 0, there is a sheaf ˜ A†,r

X on Xpro´ et such that

˜ A†,r

X (Y ) = W r(OX(Y )). Put ˜

A†

X = lim

− →r→0+ ˜ A†,r

X .

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 12 / 36

slide-30
SLIDE 30

Period sheaves I: Witt vectors and Zp-local systems

Sheaves of (overconvergent) Witt vectors

For R a perfect ring of characteristic p, the ring W (R) of Witt vectors is p-adically separated and complete and W (R)/(p) = R. Reduction modulo p admits a multiplicative section, the Teichm¨ uller map x → [x]. Proposition-Definition There is a sheaf ˜ AX on Xpro´

et such that ˜

AX(Y ) = W (OX(Y )). Proposition-Definition If R carries a power-multiplicative norm, then for r > 0, the set W r(R) of x = ∞

n=0 pn[xn] ∈ W (R) with limn→∞ pn|xn|r = 0 is a subring of W (R).

Proposition-Definition For any r > 0, there is a sheaf ˜ A†,r

X on Xpro´ et such that

˜ A†,r

X (Y ) = W r(OX(Y )). Put ˜

A†

X = lim

− →r→0+ ˜ A†,r

X .

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 12 / 36

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SLIDE 31

Period sheaves I: Witt vectors and Zp-local systems

Nonabelian Artin-Schreier theory

For S a ring and ϕ an automorphism, a ϕ-module over S is a finite projective S-module M equipped with an isomorphism ϕ∗M ∼ = M (i.e., a bijective semilinear ϕ-action). Theorem (after Katz, SGA 7) Let R be a perfect Fp-algebra. The following categories are equivalent: ´ etale Zp-local systems on Spec(R); ϕ-modules over W (R); ϕ-modules over W †(R) = ∪r>0W r(R). For R = F a field, the functors between ´ etale Zp-local systems (identified with RepZp(GF)) and ϕ-modules over W (F) are V → (V ⊗Zp W (F))GF , M → (M ⊗W (F) W (F))ϕ=1 and similarly for W †(F).

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 13 / 36

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SLIDE 32

Period sheaves I: Witt vectors and Zp-local systems

Nonabelian Artin-Schreier theory

For S a ring and ϕ an automorphism, a ϕ-module over S is a finite projective S-module M equipped with an isomorphism ϕ∗M ∼ = M (i.e., a bijective semilinear ϕ-action). Theorem (after Katz, SGA 7) Let R be a perfect Fp-algebra. The following categories are equivalent: ´ etale Zp-local systems on Spec(R); ϕ-modules over W (R); ϕ-modules over W †(R) = ∪r>0W r(R). For R = F a field, the functors between ´ etale Zp-local systems (identified with RepZp(GF)) and ϕ-modules over W (F) are V → (V ⊗Zp W (F))GF , M → (M ⊗W (F) W (F))ϕ=1 and similarly for W †(F).

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 13 / 36

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SLIDE 33

Period sheaves I: Witt vectors and Zp-local systems

Nonabelian Artin-Schreier theory

For S a ring and ϕ an automorphism, a ϕ-module over S is a finite projective S-module M equipped with an isomorphism ϕ∗M ∼ = M (i.e., a bijective semilinear ϕ-action). Theorem (after Katz, SGA 7) Let R be a perfect Fp-algebra. The following categories are equivalent: ´ etale Zp-local systems on Spec(R); ϕ-modules over W (R); ϕ-modules over W †(R) = ∪r>0W r(R). For R = F a field, the functors between ´ etale Zp-local systems (identified with RepZp(GF)) and ϕ-modules over W (F) are V → (V ⊗Zp W (F))GF , M → (M ⊗W (F) W (F))ϕ=1 and similarly for W †(F).

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 13 / 36

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SLIDE 34

Period sheaves I: Witt vectors and Zp-local systems

Nonabelian Artin-Schreier theory

For S a ring and ϕ an automorphism, a ϕ-module over S is a finite projective S-module M equipped with an isomorphism ϕ∗M ∼ = M (i.e., a bijective semilinear ϕ-action). Theorem (after Katz, SGA 7) Let R be a perfect Fp-algebra. The following categories are equivalent: ´ etale Zp-local systems on Spec(R); ϕ-modules over W (R); ϕ-modules over W †(R) = ∪r>0W r(R). For R = F a field, the functors between ´ etale Zp-local systems (identified with RepZp(GF)) and ϕ-modules over W (F) are V → (V ⊗Zp W (F))GF , M → (M ⊗W (F) W (F))ϕ=1 and similarly for W †(F).

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 13 / 36

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SLIDE 35

Period sheaves I: Witt vectors and Zp-local systems

Nonabelian Artin-Schreier theory

For S a ring and ϕ an automorphism, a ϕ-module over S is a finite projective S-module M equipped with an isomorphism ϕ∗M ∼ = M (i.e., a bijective semilinear ϕ-action). Theorem (after Katz, SGA 7) Let R be a perfect Fp-algebra. The following categories are equivalent: ´ etale Zp-local systems on Spec(R); ϕ-modules over W (R); ϕ-modules over W †(R) = ∪r>0W r(R). For R = F a field, the functors between ´ etale Zp-local systems (identified with RepZp(GF)) and ϕ-modules over W (F) are V → (V ⊗Zp W (F))GF , M → (M ⊗W (F) W (F))ϕ=1 and similarly for W †(F).

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 13 / 36

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SLIDE 36

Period sheaves I: Witt vectors and Zp-local systems

Nonabelian Artin-Schreier theory

For S a ring and ϕ an automorphism, a ϕ-module over S is a finite projective S-module M equipped with an isomorphism ϕ∗M ∼ = M (i.e., a bijective semilinear ϕ-action). Theorem (after Katz, SGA 7) Let R be a perfect Fp-algebra. The following categories are equivalent: ´ etale Zp-local systems on Spec(R); ϕ-modules over W (R); ϕ-modules over W †(R) = ∪r>0W r(R). For R = F a field, the functors between ´ etale Zp-local systems (identified with RepZp(GF)) and ϕ-modules over W (F) are V → (V ⊗Zp W (F))GF , M → (M ⊗W (F) W (F))ϕ=1 and similarly for W †(F).

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 13 / 36

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SLIDE 37

Period sheaves I: Witt vectors and Zp-local systems

Sheafified ϕ-modules

A ϕ-module over a ring sheaf ∗X on Xpro´

et is a “quasicoherent finite

projective”3 sheaf F of ∗X-modules plus an isomorphism ϕ∗F ∼ = F. Proposition Quasicoherent finite projective modules over ˜ AX

  • Y or ˜

A†

X

  • Y correspond to

finite projective modules over ˜ AX(Y ) or ˜ A†

X(Y ), respectively. Moreover,

these sheaves are acyclic.

3I.e., locally arises from a finite projective ∗X-module. Because our rings are highly

nonnoetherian, rational localizations may not be flat and so coherent sheaves cannot be handled easily, but vector bundles are no problem.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 14 / 36

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SLIDE 38

Period sheaves I: Witt vectors and Zp-local systems

Sheafified ϕ-modules

A ϕ-module over a ring sheaf ∗X on Xpro´

et is a “quasicoherent finite

projective”3 sheaf F of ∗X-modules plus an isomorphism ϕ∗F ∼ = F. Proposition Quasicoherent finite projective modules over ˜ AX

  • Y or ˜

A†

X

  • Y correspond to

finite projective modules over ˜ AX(Y ) or ˜ A†

X(Y ), respectively. Moreover,

these sheaves are acyclic.

3I.e., locally arises from a finite projective ∗X-module. Because our rings are highly

nonnoetherian, rational localizations may not be flat and so coherent sheaves cannot be handled easily, but vector bundles are no problem.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 14 / 36

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SLIDE 39

Period sheaves I: Witt vectors and Zp-local systems

Sheafified Artin-Schreier

Theorem The following categories are equivalent: ´ etale Zp-local systems on X; ϕ-modules over ˜ AX; ϕ-modules over ˜ A†

X.

The functors between ´ etale Zp-local systems and ϕ-modules over ˜ AX are T → T ⊗Zp ˜ AX, M → Mϕ=1 and similarly for ˜ A†

X.

The analogue of taking Galois invariants in the first functor is the fact that the restriction of a ϕ-module to Y is defined by a finite projective module.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 15 / 36

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SLIDE 40

Period sheaves I: Witt vectors and Zp-local systems

Sheafified Artin-Schreier

Theorem The following categories are equivalent: ´ etale Zp-local systems on X; ϕ-modules over ˜ AX; ϕ-modules over ˜ A†

X.

The functors between ´ etale Zp-local systems and ϕ-modules over ˜ AX are T → T ⊗Zp ˜ AX, M → Mϕ=1 and similarly for ˜ A†

X.

The analogue of taking Galois invariants in the first functor is the fact that the restriction of a ϕ-module to Y is defined by a finite projective module.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 15 / 36

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SLIDE 41

Period sheaves I: Witt vectors and Zp-local systems

Sheafified Artin-Schreier

Theorem The following categories are equivalent: ´ etale Zp-local systems on X; ϕ-modules over ˜ AX; ϕ-modules over ˜ A†

X.

The functors between ´ etale Zp-local systems and ϕ-modules over ˜ AX are T → T ⊗Zp ˜ AX, M → Mϕ=1 and similarly for ˜ A†

X.

The analogue of taking Galois invariants in the first functor is the fact that the restriction of a ϕ-module to Y is defined by a finite projective module.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 15 / 36

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SLIDE 42

Period sheaves I: Witt vectors and Zp-local systems

Sheafified Artin-Schreier

Theorem The following categories are equivalent: ´ etale Zp-local systems on X; ϕ-modules over ˜ AX; ϕ-modules over ˜ A†

X.

The functors between ´ etale Zp-local systems and ϕ-modules over ˜ AX are T → T ⊗Zp ˜ AX, M → Mϕ=1 and similarly for ˜ A†

X.

The analogue of taking Galois invariants in the first functor is the fact that the restriction of a ϕ-module to Y is defined by a finite projective module.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 15 / 36

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SLIDE 43

Period sheaves I: Witt vectors and Zp-local systems

Sheafified Artin-Schreier

Theorem The following categories are equivalent: ´ etale Zp-local systems on X; ϕ-modules over ˜ AX; ϕ-modules over ˜ A†

X.

The functors between ´ etale Zp-local systems and ϕ-modules over ˜ AX are T → T ⊗Zp ˜ AX, M → Mϕ=1 and similarly for ˜ A†

X.

The analogue of taking Galois invariants in the first functor is the fact that the restriction of a ϕ-module to Y is defined by a finite projective module.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 15 / 36

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SLIDE 44

Period sheaves I: Witt vectors and Zp-local systems

Sheafified Artin-Schreier

Theorem The following categories are equivalent: ´ etale Zp-local systems on X; ϕ-modules over ˜ AX; ϕ-modules over ˜ A†

X.

The functors between ´ etale Zp-local systems and ϕ-modules over ˜ AX are T → T ⊗Zp ˜ AX, M → Mϕ=1 and similarly for ˜ A†

X.

The analogue of taking Galois invariants in the first functor is the fact that the restriction of a ϕ-module to Y is defined by a finite projective module.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 15 / 36

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SLIDE 45

Period sheaves I: Witt vectors and Zp-local systems

Cohomology of Zp-local systems

By the ´ etale cohomology of a local system, we will mean the ordinary cohomology on Xpro´

et.

Theorem For T an ´ etale Zp-local system on X corresponding to a ϕ-module F over ˜ AX and a ϕ-module F† over ˜ A†

X, the sequences

0 → T → F∗ ϕ−1 → F∗ → 0 (∗ ∈ {∅, †}) are exact. The point is that F∗ is acyclic on every affinoid perfectoid, not just sufficiently small ones. (This recovers Herr’s formula for Galois cohomology of Zp-local systems over a p-adic field.)

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 16 / 36

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SLIDE 46

Period sheaves II: Robba rings and Qp-local systems

Contents

1

Overview: goals of relative p-adic Hodge theory

2

Period sheaves I: Witt vectors and Zp-local systems

3

Period sheaves II: Robba rings and Qp-local systems

4

Sheaves on relative Fargues-Fontaine curves

5

The next frontier: imperfect period rings (and maybe sheaves)

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 17 / 36

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SLIDE 47

Period sheaves II: Robba rings and Qp-local systems

An analogy

Consider the following sequence of ring constructions. A = lim ← −n→∞(Z/pnZ)((π)), a Cohen ring with residue field Fp((π)). A†,r: elements of A which converge for p−r ≤ |π| < 1. That is, for x =

n∈Z xnπn ∈ A, we have x ∈ A†,r iff limn→−∞ |xn|p−rn = 0.

A† = ∪r>0A†,r. B∗ = A∗[p−1] for ∗ ∈ {∅; †, r; †}. C[s,r]: analytic functions on the annulus p−r ≤ |π| ≤ p−s. This is the completion of Br for the max over t ∈ [s, r] (or even t = s, r) of the Gauss norm |x|t = maxn{|xn|p−tn}. Cr: analytic functions on the annulus p−r ≤ |π| < 1. This is the Fr´ echet (i.e., not uniform) completion of Br for {|•|s : 0 < s ≤ r}. C∞ = ∩r>0Cr: analytic functions on the punctured disc 0 < |π| < 1. C = ∪r>0Cr. This is commonly called the Robba ring over Qp.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 18 / 36

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SLIDE 48

Period sheaves II: Robba rings and Qp-local systems

An analogy

Consider the following sequence of ring constructions. A = lim ← −n→∞(Z/pnZ)((π)), a Cohen ring with residue field Fp((π)). A†,r: elements of A which converge for p−r ≤ |π| < 1. That is, for x =

n∈Z xnπn ∈ A, we have x ∈ A†,r iff limn→−∞ |xn|p−rn = 0.

A† = ∪r>0A†,r. B∗ = A∗[p−1] for ∗ ∈ {∅; †, r; †}. C[s,r]: analytic functions on the annulus p−r ≤ |π| ≤ p−s. This is the completion of Br for the max over t ∈ [s, r] (or even t = s, r) of the Gauss norm |x|t = maxn{|xn|p−tn}. Cr: analytic functions on the annulus p−r ≤ |π| < 1. This is the Fr´ echet (i.e., not uniform) completion of Br for {|•|s : 0 < s ≤ r}. C∞ = ∩r>0Cr: analytic functions on the punctured disc 0 < |π| < 1. C = ∪r>0Cr. This is commonly called the Robba ring over Qp.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 18 / 36

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SLIDE 49

Period sheaves II: Robba rings and Qp-local systems

An analogy

Consider the following sequence of ring constructions. A = lim ← −n→∞(Z/pnZ)((π)), a Cohen ring with residue field Fp((π)). A†,r: elements of A which converge for p−r ≤ |π| < 1. That is, for x =

n∈Z xnπn ∈ A, we have x ∈ A†,r iff limn→−∞ |xn|p−rn = 0.

A† = ∪r>0A†,r. B∗ = A∗[p−1] for ∗ ∈ {∅; †, r; †}. C[s,r]: analytic functions on the annulus p−r ≤ |π| ≤ p−s. This is the completion of Br for the max over t ∈ [s, r] (or even t = s, r) of the Gauss norm |x|t = maxn{|xn|p−tn}. Cr: analytic functions on the annulus p−r ≤ |π| < 1. This is the Fr´ echet (i.e., not uniform) completion of Br for {|•|s : 0 < s ≤ r}. C∞ = ∩r>0Cr: analytic functions on the punctured disc 0 < |π| < 1. C = ∪r>0Cr. This is commonly called the Robba ring over Qp.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 18 / 36

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SLIDE 50

Period sheaves II: Robba rings and Qp-local systems

An analogy

Consider the following sequence of ring constructions. A = lim ← −n→∞(Z/pnZ)((π)), a Cohen ring with residue field Fp((π)). A†,r: elements of A which converge for p−r ≤ |π| < 1. That is, for x =

n∈Z xnπn ∈ A, we have x ∈ A†,r iff limn→−∞ |xn|p−rn = 0.

A† = ∪r>0A†,r. B∗ = A∗[p−1] for ∗ ∈ {∅; †, r; †}. C[s,r]: analytic functions on the annulus p−r ≤ |π| ≤ p−s. This is the completion of Br for the max over t ∈ [s, r] (or even t = s, r) of the Gauss norm |x|t = maxn{|xn|p−tn}. Cr: analytic functions on the annulus p−r ≤ |π| < 1. This is the Fr´ echet (i.e., not uniform) completion of Br for {|•|s : 0 < s ≤ r}. C∞ = ∩r>0Cr: analytic functions on the punctured disc 0 < |π| < 1. C = ∪r>0Cr. This is commonly called the Robba ring over Qp.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 18 / 36

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SLIDE 51

Period sheaves II: Robba rings and Qp-local systems

An analogy

Consider the following sequence of ring constructions. A = lim ← −n→∞(Z/pnZ)((π)), a Cohen ring with residue field Fp((π)). A†,r: elements of A which converge for p−r ≤ |π| < 1. That is, for x =

n∈Z xnπn ∈ A, we have x ∈ A†,r iff limn→−∞ |xn|p−rn = 0.

A† = ∪r>0A†,r. B∗ = A∗[p−1] for ∗ ∈ {∅; †, r; †}. C[s,r]: analytic functions on the annulus p−r ≤ |π| ≤ p−s. This is the completion of Br for the max over t ∈ [s, r] (or even t = s, r) of the Gauss norm |x|t = maxn{|xn|p−tn}. Cr: analytic functions on the annulus p−r ≤ |π| < 1. This is the Fr´ echet (i.e., not uniform) completion of Br for {|•|s : 0 < s ≤ r}. C∞ = ∩r>0Cr: analytic functions on the punctured disc 0 < |π| < 1. C = ∪r>0Cr. This is commonly called the Robba ring over Qp.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 18 / 36

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SLIDE 52

Period sheaves II: Robba rings and Qp-local systems

An analogy

Consider the following sequence of ring constructions. A = lim ← −n→∞(Z/pnZ)((π)), a Cohen ring with residue field Fp((π)). A†,r: elements of A which converge for p−r ≤ |π| < 1. That is, for x =

n∈Z xnπn ∈ A, we have x ∈ A†,r iff limn→−∞ |xn|p−rn = 0.

A† = ∪r>0A†,r. B∗ = A∗[p−1] for ∗ ∈ {∅; †, r; †}. C[s,r]: analytic functions on the annulus p−r ≤ |π| ≤ p−s. This is the completion of Br for the max over t ∈ [s, r] (or even t = s, r) of the Gauss norm |x|t = maxn{|xn|p−tn}. Cr: analytic functions on the annulus p−r ≤ |π| < 1. This is the Fr´ echet (i.e., not uniform) completion of Br for {|•|s : 0 < s ≤ r}. C∞ = ∩r>0Cr: analytic functions on the punctured disc 0 < |π| < 1. C = ∪r>0Cr. This is commonly called the Robba ring over Qp.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 18 / 36

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SLIDE 53

Period sheaves II: Robba rings and Qp-local systems

An analogy

Consider the following sequence of ring constructions. A = lim ← −n→∞(Z/pnZ)((π)), a Cohen ring with residue field Fp((π)). A†,r: elements of A which converge for p−r ≤ |π| < 1. That is, for x =

n∈Z xnπn ∈ A, we have x ∈ A†,r iff limn→−∞ |xn|p−rn = 0.

A† = ∪r>0A†,r. B∗ = A∗[p−1] for ∗ ∈ {∅; †, r; †}. C[s,r]: analytic functions on the annulus p−r ≤ |π| ≤ p−s. This is the completion of Br for the max over t ∈ [s, r] (or even t = s, r) of the Gauss norm |x|t = maxn{|xn|p−tn}. Cr: analytic functions on the annulus p−r ≤ |π| < 1. This is the Fr´ echet (i.e., not uniform) completion of Br for {|•|s : 0 < s ≤ r}. C∞ = ∩r>0Cr: analytic functions on the punctured disc 0 < |π| < 1. C = ∪r>0Cr. This is commonly called the Robba ring over Qp.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 18 / 36

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SLIDE 54

Period sheaves II: Robba rings and Qp-local systems

An analogy

Consider the following sequence of ring constructions. A = lim ← −n→∞(Z/pnZ)((π)), a Cohen ring with residue field Fp((π)). A†,r: elements of A which converge for p−r ≤ |π| < 1. That is, for x =

n∈Z xnπn ∈ A, we have x ∈ A†,r iff limn→−∞ |xn|p−rn = 0.

A† = ∪r>0A†,r. B∗ = A∗[p−1] for ∗ ∈ {∅; †, r; †}. C[s,r]: analytic functions on the annulus p−r ≤ |π| ≤ p−s. This is the completion of Br for the max over t ∈ [s, r] (or even t = s, r) of the Gauss norm |x|t = maxn{|xn|p−tn}. Cr: analytic functions on the annulus p−r ≤ |π| < 1. This is the Fr´ echet (i.e., not uniform) completion of Br for {|•|s : 0 < s ≤ r}. C∞ = ∩r>0Cr: analytic functions on the punctured disc 0 < |π| < 1. C = ∪r>0Cr. This is commonly called the Robba ring over Qp.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 18 / 36

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SLIDE 55

Period sheaves II: Robba rings and Qp-local systems

An analogy

Consider the following sequence of ring constructions. A = lim ← −n→∞(Z/pnZ)((π)), a Cohen ring with residue field Fp((π)). A†,r: elements of A which converge for p−r ≤ |π| < 1. That is, for x =

n∈Z xnπn ∈ A, we have x ∈ A†,r iff limn→−∞ |xn|p−rn = 0.

A† = ∪r>0A†,r. B∗ = A∗[p−1] for ∗ ∈ {∅; †, r; †}. C[s,r]: analytic functions on the annulus p−r ≤ |π| ≤ p−s. This is the completion of Br for the max over t ∈ [s, r] (or even t = s, r) of the Gauss norm |x|t = maxn{|xn|p−tn}. Cr: analytic functions on the annulus p−r ≤ |π| < 1. This is the Fr´ echet (i.e., not uniform) completion of Br for {|•|s : 0 < s ≤ r}. C∞ = ∩r>0Cr: analytic functions on the punctured disc 0 < |π| < 1. C = ∪r>0Cr. This is commonly called the Robba ring over Qp.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 18 / 36

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SLIDE 56

Period sheaves II: Robba rings and Qp-local systems

Some more period sheaves

Following the previous analogy, we now define some more sheaves. Proposition-Definition There exist sheaves on Xpro´

et with the following sections.

˜ B∗(Y ) = ˜ A∗(Y ) for ∗ ∈ {∅; †, r; †}. ˜ C[s,r](Y ) is the completion of ˜ Br(Y ) for the maximum over t ∈ [s, r] (or even t = s, r) of the Gauss norm |x|t = maxn{p−n|xn|r}. Note that ϕ : ˜ C[s,r](Y ) → ˜ C[s/p,r/p](Y ) is an isomorphism. (This is one of the rings BA,E,I of the talks of Fargues and Fontaine with E = Qp.) ˜ Cr(Y ) is the Fr´ echet completion of ˜ Br(Y ) for {|•|s : 0 < s ≤ r}. Similarly, ϕ : ˜ Cr(Y ) → ˜ Cr/p(Y ) is an isomorphism. ˜ C∞(Y ) = ∩r>0˜ Cr(Y ) = lim ← −r→0+ ˜ Cr(Y ). ˜ C(Y ) = ∪r>0˜ Cr(Y ) = lim − →r→0+ ˜ Cr(Y ).

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 19 / 36

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SLIDE 57

Period sheaves II: Robba rings and Qp-local systems

Some more period sheaves

Following the previous analogy, we now define some more sheaves. Proposition-Definition There exist sheaves on Xpro´

et with the following sections.

˜ B∗(Y ) = ˜ A∗(Y ) for ∗ ∈ {∅; †, r; †}. ˜ C[s,r](Y ) is the completion of ˜ Br(Y ) for the maximum over t ∈ [s, r] (or even t = s, r) of the Gauss norm |x|t = maxn{p−n|xn|r}. Note that ϕ : ˜ C[s,r](Y ) → ˜ C[s/p,r/p](Y ) is an isomorphism. (This is one of the rings BA,E,I of the talks of Fargues and Fontaine with E = Qp.) ˜ Cr(Y ) is the Fr´ echet completion of ˜ Br(Y ) for {|•|s : 0 < s ≤ r}. Similarly, ϕ : ˜ Cr(Y ) → ˜ Cr/p(Y ) is an isomorphism. ˜ C∞(Y ) = ∩r>0˜ Cr(Y ) = lim ← −r→0+ ˜ Cr(Y ). ˜ C(Y ) = ∪r>0˜ Cr(Y ) = lim − →r→0+ ˜ Cr(Y ).

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 19 / 36

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SLIDE 58

Period sheaves II: Robba rings and Qp-local systems

Some more period sheaves

Following the previous analogy, we now define some more sheaves. Proposition-Definition There exist sheaves on Xpro´

et with the following sections.

˜ B∗(Y ) = ˜ A∗(Y ) for ∗ ∈ {∅; †, r; †}. ˜ C[s,r](Y ) is the completion of ˜ Br(Y ) for the maximum over t ∈ [s, r] (or even t = s, r) of the Gauss norm |x|t = maxn{p−n|xn|r}. Note that ϕ : ˜ C[s,r](Y ) → ˜ C[s/p,r/p](Y ) is an isomorphism. (This is one of the rings BA,E,I of the talks of Fargues and Fontaine with E = Qp.) ˜ Cr(Y ) is the Fr´ echet completion of ˜ Br(Y ) for {|•|s : 0 < s ≤ r}. Similarly, ϕ : ˜ Cr(Y ) → ˜ Cr/p(Y ) is an isomorphism. ˜ C∞(Y ) = ∩r>0˜ Cr(Y ) = lim ← −r→0+ ˜ Cr(Y ). ˜ C(Y ) = ∪r>0˜ Cr(Y ) = lim − →r→0+ ˜ Cr(Y ).

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 19 / 36

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SLIDE 59

Period sheaves II: Robba rings and Qp-local systems

Some more period sheaves

Following the previous analogy, we now define some more sheaves. Proposition-Definition There exist sheaves on Xpro´

et with the following sections.

˜ B∗(Y ) = ˜ A∗(Y ) for ∗ ∈ {∅; †, r; †}. ˜ C[s,r](Y ) is the completion of ˜ Br(Y ) for the maximum over t ∈ [s, r] (or even t = s, r) of the Gauss norm |x|t = maxn{p−n|xn|r}. Note that ϕ : ˜ C[s,r](Y ) → ˜ C[s/p,r/p](Y ) is an isomorphism. (This is one of the rings BA,E,I of the talks of Fargues and Fontaine with E = Qp.) ˜ Cr(Y ) is the Fr´ echet completion of ˜ Br(Y ) for {|•|s : 0 < s ≤ r}. Similarly, ϕ : ˜ Cr(Y ) → ˜ Cr/p(Y ) is an isomorphism. ˜ C∞(Y ) = ∩r>0˜ Cr(Y ) = lim ← −r→0+ ˜ Cr(Y ). ˜ C(Y ) = ∪r>0˜ Cr(Y ) = lim − →r→0+ ˜ Cr(Y ).

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 19 / 36

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SLIDE 60

Period sheaves II: Robba rings and Qp-local systems

Some more period sheaves

Following the previous analogy, we now define some more sheaves. Proposition-Definition There exist sheaves on Xpro´

et with the following sections.

˜ B∗(Y ) = ˜ A∗(Y ) for ∗ ∈ {∅; †, r; †}. ˜ C[s,r](Y ) is the completion of ˜ Br(Y ) for the maximum over t ∈ [s, r] (or even t = s, r) of the Gauss norm |x|t = maxn{p−n|xn|r}. Note that ϕ : ˜ C[s,r](Y ) → ˜ C[s/p,r/p](Y ) is an isomorphism. (This is one of the rings BA,E,I of the talks of Fargues and Fontaine with E = Qp.) ˜ Cr(Y ) is the Fr´ echet completion of ˜ Br(Y ) for {|•|s : 0 < s ≤ r}. Similarly, ϕ : ˜ Cr(Y ) → ˜ Cr/p(Y ) is an isomorphism. ˜ C∞(Y ) = ∩r>0˜ Cr(Y ) = lim ← −r→0+ ˜ Cr(Y ). ˜ C(Y ) = ∪r>0˜ Cr(Y ) = lim − →r→0+ ˜ Cr(Y ).

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 19 / 36

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SLIDE 61

Period sheaves II: Robba rings and Qp-local systems

Some more period sheaves

Following the previous analogy, we now define some more sheaves. Proposition-Definition There exist sheaves on Xpro´

et with the following sections.

˜ B∗(Y ) = ˜ A∗(Y ) for ∗ ∈ {∅; †, r; †}. ˜ C[s,r](Y ) is the completion of ˜ Br(Y ) for the maximum over t ∈ [s, r] (or even t = s, r) of the Gauss norm |x|t = maxn{p−n|xn|r}. Note that ϕ : ˜ C[s,r](Y ) → ˜ C[s/p,r/p](Y ) is an isomorphism. (This is one of the rings BA,E,I of the talks of Fargues and Fontaine with E = Qp.) ˜ Cr(Y ) is the Fr´ echet completion of ˜ Br(Y ) for {|•|s : 0 < s ≤ r}. Similarly, ϕ : ˜ Cr(Y ) → ˜ Cr/p(Y ) is an isomorphism. ˜ C∞(Y ) = ∩r>0˜ Cr(Y ) = lim ← −r→0+ ˜ Cr(Y ). ˜ C(Y ) = ∪r>0˜ Cr(Y ) = lim − →r→0+ ˜ Cr(Y ).

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 19 / 36

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SLIDE 62

Period sheaves II: Robba rings and Qp-local systems

Some more period sheaves

Following the previous analogy, we now define some more sheaves. Proposition-Definition There exist sheaves on Xpro´

et with the following sections.

˜ B∗(Y ) = ˜ A∗(Y ) for ∗ ∈ {∅; †, r; †}. ˜ C[s,r](Y ) is the completion of ˜ Br(Y ) for the maximum over t ∈ [s, r] (or even t = s, r) of the Gauss norm |x|t = maxn{p−n|xn|r}. Note that ϕ : ˜ C[s,r](Y ) → ˜ C[s/p,r/p](Y ) is an isomorphism. (This is one of the rings BA,E,I of the talks of Fargues and Fontaine with E = Qp.) ˜ Cr(Y ) is the Fr´ echet completion of ˜ Br(Y ) for {|•|s : 0 < s ≤ r}. Similarly, ϕ : ˜ Cr(Y ) → ˜ Cr/p(Y ) is an isomorphism. ˜ C∞(Y ) = ∩r>0˜ Cr(Y ) = lim ← −r→0+ ˜ Cr(Y ). ˜ C(Y ) = ∪r>0˜ Cr(Y ) = lim − →r→0+ ˜ Cr(Y ).

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 19 / 36

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SLIDE 63

Period sheaves II: Robba rings and Qp-local systems

ϕ-modules over ˜ CX

A ϕ-module over ˜ CX is ´ etale at x ∈ X if adic-locally around x it arises by base extension from a ϕ-module over ˜ A†

X.

Theorem The ´ etale condition is pointwise: it suffices to check it after pullback to the one-point space x. Theorem The slope polygon (to be defined later) of any ϕ-module is a lower semicontinuous function on X (with locally constant endpoints). If X arose from a Berkovich space, this is also true for Berkovich’s topology (i.e., on the maximal Hausdorff quotient of X).

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 20 / 36

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SLIDE 64

Period sheaves II: Robba rings and Qp-local systems

ϕ-modules over ˜ CX

A ϕ-module over ˜ CX is ´ etale at x ∈ X if adic-locally around x it arises by base extension from a ϕ-module over ˜ A†

X.

Theorem The ´ etale condition is pointwise: it suffices to check it after pullback to the one-point space x. Theorem The slope polygon (to be defined later) of any ϕ-module is a lower semicontinuous function on X (with locally constant endpoints). If X arose from a Berkovich space, this is also true for Berkovich’s topology (i.e., on the maximal Hausdorff quotient of X).

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 20 / 36

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SLIDE 65

Period sheaves II: Robba rings and Qp-local systems

ϕ-modules over ˜ CX

A ϕ-module over ˜ CX is ´ etale at x ∈ X if adic-locally around x it arises by base extension from a ϕ-module over ˜ A†

X.

Theorem The ´ etale condition is pointwise: it suffices to check it after pullback to the one-point space x. Theorem The slope polygon (to be defined later) of any ϕ-module is a lower semicontinuous function on X (with locally constant endpoints). If X arose from a Berkovich space, this is also true for Berkovich’s topology (i.e., on the maximal Hausdorff quotient of X).

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 20 / 36

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SLIDE 66

Period sheaves II: Robba rings and Qp-local systems

Globalized Artin-Schreier

Theorem The following categories are equivalent: ´ etale Qp-local systems on X; ´ etale ϕ-modules over ˜ CX. ´ etale ϕ-modules over ˜ C∞

X .

Also, for V an ´ etale Qp-local system on X corresponding to a ϕ-module F

  • ver ˜

C∗

X, for ∗ ∈ {∅, ∞}, the sequence

0 → V → F

ϕ−1

→ F → 0 is exact. (And again F is acyclic over every Y .)

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 21 / 36

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SLIDE 67

Period sheaves II: Robba rings and Qp-local systems

Globalized Artin-Schreier

Theorem The following categories are equivalent: ´ etale Qp-local systems on X; ´ etale ϕ-modules over ˜ CX. ´ etale ϕ-modules over ˜ C∞

X .

Also, for V an ´ etale Qp-local system on X corresponding to a ϕ-module F

  • ver ˜

C∗

X, for ∗ ∈ {∅, ∞}, the sequence

0 → V → F

ϕ−1

→ F → 0 is exact. (And again F is acyclic over every Y .)

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 21 / 36

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SLIDE 68

Period sheaves II: Robba rings and Qp-local systems

Globalized Artin-Schreier

Theorem The following categories are equivalent: ´ etale Qp-local systems on X; ´ etale ϕ-modules over ˜ CX. ´ etale ϕ-modules over ˜ C∞

X .

Also, for V an ´ etale Qp-local system on X corresponding to a ϕ-module F

  • ver ˜

C∗

X, for ∗ ∈ {∅, ∞}, the sequence

0 → V → F

ϕ−1

→ F → 0 is exact. (And again F is acyclic over every Y .)

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 21 / 36

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SLIDE 69

Period sheaves II: Robba rings and Qp-local systems

Globalized Artin-Schreier

Theorem The following categories are equivalent: ´ etale Qp-local systems on X; ´ etale ϕ-modules over ˜ CX. ´ etale ϕ-modules over ˜ C∞

X .

Also, for V an ´ etale Qp-local system on X corresponding to a ϕ-module F

  • ver ˜

C∗

X, for ∗ ∈ {∅, ∞}, the sequence

0 → V → F

ϕ−1

→ F → 0 is exact. (And again F is acyclic over every Y .)

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 21 / 36

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SLIDE 70

Period sheaves II: Robba rings and Qp-local systems

Globalized Artin-Schreier

Theorem The following categories are equivalent: ´ etale Qp-local systems on X; ´ etale ϕ-modules over ˜ CX. ´ etale ϕ-modules over ˜ C∞

X .

Also, for V an ´ etale Qp-local system on X corresponding to a ϕ-module F

  • ver ˜

C∗

X, for ∗ ∈ {∅, ∞}, the sequence

0 → V → F

ϕ−1

→ F → 0 is exact. (And again F is acyclic over every Y .)

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 21 / 36

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SLIDE 71

Period sheaves II: Robba rings and Qp-local systems

Future attractions: removing the puncture

One can also define sheaves ˜ A+

X, ˜

B+

X, ˜

C+

X where ˜

A+

X(Y ) = W (O(Y )+).

This is analogous to taking the whole unit disc, without a puncture. One can define “Wach-Breuil-Kisin modules” over ˜ A+

X where the action of

ϕ is not bijective, but has controlled kernel and cokernel. These give rise to what we should call crystalline ϕ-modules over ˜ CX. But beware: this construction depends heavily on the + subrings!

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 22 / 36

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SLIDE 72

Period sheaves II: Robba rings and Qp-local systems

Future attractions: removing the puncture

One can also define sheaves ˜ A+

X, ˜

B+

X, ˜

C+

X where ˜

A+

X(Y ) = W (O(Y )+).

This is analogous to taking the whole unit disc, without a puncture. One can define “Wach-Breuil-Kisin modules” over ˜ A+

X where the action of

ϕ is not bijective, but has controlled kernel and cokernel. These give rise to what we should call crystalline ϕ-modules over ˜ CX. But beware: this construction depends heavily on the + subrings!

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 22 / 36

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SLIDE 73

Period sheaves II: Robba rings and Qp-local systems

Future attractions: removing the puncture

One can also define sheaves ˜ A+

X, ˜

B+

X, ˜

C+

X where ˜

A+

X(Y ) = W (O(Y )+).

This is analogous to taking the whole unit disc, without a puncture. One can define “Wach-Breuil-Kisin modules” over ˜ A+

X where the action of

ϕ is not bijective, but has controlled kernel and cokernel. These give rise to what we should call crystalline ϕ-modules over ˜ CX. But beware: this construction depends heavily on the + subrings!

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 22 / 36

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SLIDE 74

Sheaves on relative Fargues-Fontaine curves

Contents

1

Overview: goals of relative p-adic Hodge theory

2

Period sheaves I: Witt vectors and Zp-local systems

3

Period sheaves II: Robba rings and Qp-local systems

4

Sheaves on relative Fargues-Fontaine curves

5

The next frontier: imperfect period rings (and maybe sheaves)

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 23 / 36

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SLIDE 75

Sheaves on relative Fargues-Fontaine curves

Disclaimer

In this section, we take X to be perfectoid (over Qp), but not necessarily

  • ver a perfectoid field. Now Y is an arbitrary affinoid perfectoid subspace
  • f X (since Xpro´

et is tricky).

The relative curve we consider is the one from the lecture of Fargues, but for this exposition we only take E = Qp and q = p.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 24 / 36

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SLIDE 76

Sheaves on relative Fargues-Fontaine curves

Disclaimer

In this section, we take X to be perfectoid (over Qp), but not necessarily

  • ver a perfectoid field. Now Y is an arbitrary affinoid perfectoid subspace
  • f X (since Xpro´

et is tricky).

The relative curve we consider is the one from the lecture of Fargues, but for this exposition we only take E = Qp and q = p.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 24 / 36

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SLIDE 77

Sheaves on relative Fargues-Fontaine curves

The construction over an affinoid perfectoid

Pick any r > 0. The relative Fargues-Fontaine curve FFY is obtained4 from the “annulus” Spa(˜ C[r/p,r]

X

(Y )) by glueing the “edges” Spa(˜ C[r/p,r/p]

X

(Y )) and Spa(˜ C[r,r]

X

(Y )) via ϕ. This is independent of r. There is also an algebraic analogue: FFalg

Y = Proj(PY ),

PY =

  • n=0

˜ CX(Y )ϕ=pn. Theorem There is a natural morphism FFY → FFalg

Y

  • f locally ringed spaces which

induces an equivalence of categories of vector bundles. Moreover, these categories are equivalent to ϕ-modules over ˜ CY and ˜ C∞

Y . (Again, we don’t

consider coherent sheaves due to non-noetherianity.)

4We’ve omitted the second inputs into Spa for brevity. Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 25 / 36

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SLIDE 78

Sheaves on relative Fargues-Fontaine curves

The construction over an affinoid perfectoid

Pick any r > 0. The relative Fargues-Fontaine curve FFY is obtained4 from the “annulus” Spa(˜ C[r/p,r]

X

(Y )) by glueing the “edges” Spa(˜ C[r/p,r/p]

X

(Y )) and Spa(˜ C[r,r]

X

(Y )) via ϕ. This is independent of r. There is also an algebraic analogue: FFalg

Y = Proj(PY ),

PY =

  • n=0

˜ CX(Y )ϕ=pn. Theorem There is a natural morphism FFY → FFalg

Y

  • f locally ringed spaces which

induces an equivalence of categories of vector bundles. Moreover, these categories are equivalent to ϕ-modules over ˜ CY and ˜ C∞

Y . (Again, we don’t

consider coherent sheaves due to non-noetherianity.)

4We’ve omitted the second inputs into Spa for brevity. Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 25 / 36

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SLIDE 79

Sheaves on relative Fargues-Fontaine curves

Slopes over a perfectoid field

Suppose X = Spa(K, K +) for K a perfectoid field; then FFX is the Fargues-Fontaine adic curve associated to K ♭. The algebraic curve FFalg

X

is a noetherian scheme of dimension 1 with a morphism deg : Pic(FFX) = Pic(FFalg

X ) → Z taking O(1) to 1.

For any nonzero vector bundle F on FFX, set deg(F) = deg(∧rank(F)F). The slope of F is µ(F) = deg(F)/ rank(F). We say F is semistable if µ(F) ≥ µ(G) for any proper nonzero subbundle G of F.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 26 / 36

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SLIDE 80

Sheaves on relative Fargues-Fontaine curves

Slopes over a perfectoid field

Suppose X = Spa(K, K +) for K a perfectoid field; then FFX is the Fargues-Fontaine adic curve associated to K ♭. The algebraic curve FFalg

X

is a noetherian scheme of dimension 1 with a morphism deg : Pic(FFX) = Pic(FFalg

X ) → Z taking O(1) to 1.

For any nonzero vector bundle F on FFX, set deg(F) = deg(∧rank(F)F). The slope of F is µ(F) = deg(F)/ rank(F). We say F is semistable if µ(F) ≥ µ(G) for any proper nonzero subbundle G of F.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 26 / 36

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SLIDE 81

Sheaves on relative Fargues-Fontaine curves

Slopes over a perfectoid field

Suppose X = Spa(K, K +) for K a perfectoid field; then FFX is the Fargues-Fontaine adic curve associated to K ♭. The algebraic curve FFalg

X

is a noetherian scheme of dimension 1 with a morphism deg : Pic(FFX) = Pic(FFalg

X ) → Z taking O(1) to 1.

For any nonzero vector bundle F on FFX, set deg(F) = deg(∧rank(F)F). The slope of F is µ(F) = deg(F)/ rank(F). We say F is semistable if µ(F) ≥ µ(G) for any proper nonzero subbundle G of F.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 26 / 36

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SLIDE 82

Sheaves on relative Fargues-Fontaine curves

Slopes over a perfectoid field

Suppose X = Spa(K, K +) for K a perfectoid field; then FFX is the Fargues-Fontaine adic curve associated to K ♭. The algebraic curve FFalg

X

is a noetherian scheme of dimension 1 with a morphism deg : Pic(FFX) = Pic(FFalg

X ) → Z taking O(1) to 1.

For any nonzero vector bundle F on FFX, set deg(F) = deg(∧rank(F)F). The slope of F is µ(F) = deg(F)/ rank(F). We say F is semistable if µ(F) ≥ µ(G) for any proper nonzero subbundle G of F.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 26 / 36

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SLIDE 83

Sheaves on relative Fargues-Fontaine curves

Slopes over a perfectoid field (contd.)

Suppose X = Spa(K, K +) for K a perfectoid field. Theorem (K, Fargues-Fontaine, et al.) If K is algebraically closed, then every vector bundle on FFX splits as a direct sum ⊕n

i=1O(ri/si) for some ri/si ∈ Q. (Here O(ri/si) is the

pushforward of O(ri) along the finite ´ etale map from the curve with q = psi.) Theorem A ϕ-module over ˜ CX is ´ etale iff the corresponding vector bundle on FFX is semistable of degree 0. Theorem The tensor product of two semistable vector bundles on FFX is again semistable.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 27 / 36

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SLIDE 84

Sheaves on relative Fargues-Fontaine curves

Slopes over a perfectoid field (contd.)

Suppose X = Spa(K, K +) for K a perfectoid field. Theorem (K, Fargues-Fontaine, et al.) If K is algebraically closed, then every vector bundle on FFX splits as a direct sum ⊕n

i=1O(ri/si) for some ri/si ∈ Q. (Here O(ri/si) is the

pushforward of O(ri) along the finite ´ etale map from the curve with q = psi.) Theorem A ϕ-module over ˜ CX is ´ etale iff the corresponding vector bundle on FFX is semistable of degree 0. Theorem The tensor product of two semistable vector bundles on FFX is again semistable.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 27 / 36

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SLIDE 85

Sheaves on relative Fargues-Fontaine curves

Slopes over a perfectoid field (contd.)

Suppose X = Spa(K, K +) for K a perfectoid field. Theorem (K, Fargues-Fontaine, et al.) If K is algebraically closed, then every vector bundle on FFX splits as a direct sum ⊕n

i=1O(ri/si) for some ri/si ∈ Q. (Here O(ri/si) is the

pushforward of O(ri) along the finite ´ etale map from the curve with q = psi.) Theorem A ϕ-module over ˜ CX is ´ etale iff the corresponding vector bundle on FFX is semistable of degree 0. Theorem The tensor product of two semistable vector bundles on FFX is again semistable.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 27 / 36

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SLIDE 86

Sheaves on relative Fargues-Fontaine curves

Slope filtrations over a perfectoid field

Suppose X = Spa(K, K +) for K a perfectoid field. Then every vector bundle F on FFX admits a unique Harder-Narasimhan filtration 0 = F0 ⊂ · · · ⊂ Fm = F such that each Fi/Fi−1 is a nonzero vector bundle which is semistable of slope µi and µ1 > · · · > µm. The slope polygon of F is the Newton polygon having slope µi with multiplicity rank(Fi/Fi−1). This is flat iff F is semistable.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 28 / 36

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SLIDE 87

Sheaves on relative Fargues-Fontaine curves

Slope filtrations over a perfectoid field

Suppose X = Spa(K, K +) for K a perfectoid field. Then every vector bundle F on FFX admits a unique Harder-Narasimhan filtration 0 = F0 ⊂ · · · ⊂ Fm = F such that each Fi/Fi−1 is a nonzero vector bundle which is semistable of slope µi and µ1 > · · · > µm. The slope polygon of F is the Newton polygon having slope µi with multiplicity rank(Fi/Fi−1). This is flat iff F is semistable.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 28 / 36

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SLIDE 88

Sheaves on relative Fargues-Fontaine curves

A family of curves, in a sense

For general X, we may glue the adic (but not the algebraic) construction. Theorem For X perfectoid, the spaces FFY glue to give an adic space FFX over Qp which is preperfectoid (its base extension from Qp to any perfectoid field is perfectoid). The vector bundles on FFX correspond to ϕ-modules over ˜

  • CX. Everything is functorial in X (and so far even in X ♭).

In a certain sense, the space FFX is a family of Fargues-Fontaine curves. Theorem There is a natural continuous map |FFX| → |X| whose formation is functorial in X. (But it doesn’t naturally arise from a map of adic spaces!)

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 29 / 36

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SLIDE 89

Sheaves on relative Fargues-Fontaine curves

A family of curves, in a sense

For general X, we may glue the adic (but not the algebraic) construction. Theorem For X perfectoid, the spaces FFY glue to give an adic space FFX over Qp which is preperfectoid (its base extension from Qp to any perfectoid field is perfectoid). The vector bundles on FFX correspond to ϕ-modules over ˜

  • CX. Everything is functorial in X (and so far even in X ♭).

In a certain sense, the space FFX is a family of Fargues-Fontaine curves. Theorem There is a natural continuous map |FFX| → |X| whose formation is functorial in X. (But it doesn’t naturally arise from a map of adic spaces!)

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 29 / 36

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SLIDE 90

Sheaves on relative Fargues-Fontaine curves

A family of curves, in a sense

For general X, we may glue the adic (but not the algebraic) construction. Theorem For X perfectoid, the spaces FFY glue to give an adic space FFX over Qp which is preperfectoid (its base extension from Qp to any perfectoid field is perfectoid). The vector bundles on FFX correspond to ϕ-modules over ˜

  • CX. Everything is functorial in X (and so far even in X ♭).

In a certain sense, the space FFX is a family of Fargues-Fontaine curves. Theorem There is a natural continuous map |FFX| → |X| whose formation is functorial in X. (But it doesn’t naturally arise from a map of adic spaces!)

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 29 / 36

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SLIDE 91

Sheaves on relative Fargues-Fontaine curves

A family of curves, in a sense

For general X, we may glue the adic (but not the algebraic) construction. Theorem For X perfectoid, the spaces FFY glue to give an adic space FFX over Qp which is preperfectoid (its base extension from Qp to any perfectoid field is perfectoid). The vector bundles on FFX correspond to ϕ-modules over ˜

  • CX. Everything is functorial in X (and so far even in X ♭).

In a certain sense, the space FFX is a family of Fargues-Fontaine curves. Theorem There is a natural continuous map |FFX| → |X| whose formation is functorial in X. (But it doesn’t naturally arise from a map of adic spaces!)

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 29 / 36

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SLIDE 92

Sheaves on relative Fargues-Fontaine curves

Local systems revisited

Combining previous statements, we get the following. Theorem For X perfectoid, ´ etale Qp-local systems on X form a category equivalent to vector bundles on FFX which are fiberwise semistable of degree 0. Moreover, the ´ etale cohomology of a local system coincides with the coherent cohomology of the corresponding vector bundle. Theorem The slope polygon of a vector bundle on FFX is upper semicontinuous as a function on |X| (with locally constant endpoints). This remains true on the maximal Hausdorff quotient of |X| provided that X is taut (closures

  • f quasicompact opens are quasicompact).

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 30 / 36

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SLIDE 93

Sheaves on relative Fargues-Fontaine curves

Local systems revisited

Combining previous statements, we get the following. Theorem For X perfectoid, ´ etale Qp-local systems on X form a category equivalent to vector bundles on FFX which are fiberwise semistable of degree 0. Moreover, the ´ etale cohomology of a local system coincides with the coherent cohomology of the corresponding vector bundle. Theorem The slope polygon of a vector bundle on FFX is upper semicontinuous as a function on |X| (with locally constant endpoints). This remains true on the maximal Hausdorff quotient of |X| provided that X is taut (closures

  • f quasicompact opens are quasicompact).

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 30 / 36

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SLIDE 94

Sheaves on relative Fargues-Fontaine curves

Local systems revisited

Combining previous statements, we get the following. Theorem For X perfectoid, ´ etale Qp-local systems on X form a category equivalent to vector bundles on FFX which are fiberwise semistable of degree 0. Moreover, the ´ etale cohomology of a local system coincides with the coherent cohomology of the corresponding vector bundle. Theorem The slope polygon of a vector bundle on FFX is upper semicontinuous as a function on |X| (with locally constant endpoints). This remains true on the maximal Hausdorff quotient of |X| provided that X is taut (closures

  • f quasicompact opens are quasicompact).

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 30 / 36

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SLIDE 95

Sheaves on relative Fargues-Fontaine curves

Ampleness for vector bundles

A vector bundle F on FFX is ample if for any vector bundle G on FFY , G ⊗ F⊗n is generated by global sections for n ≫ 0. Theorem O(1) is ample. Consequently, to check ampleness we need only consider G = O(d) for d ∈ Z (over all Y ; the powers of F need not be uniform). Theorem F is ample iff for all Y and d, H1(FFY , F⊗n(d)) = 0 for n ≫ 0. Theorem F is ample iff its slopes are everywhere positive. Consequently, this condition is pointwise and open on |X|.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 31 / 36

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SLIDE 96

Sheaves on relative Fargues-Fontaine curves

Ampleness for vector bundles

A vector bundle F on FFX is ample if for any vector bundle G on FFY , G ⊗ F⊗n is generated by global sections for n ≫ 0. Theorem O(1) is ample. Consequently, to check ampleness we need only consider G = O(d) for d ∈ Z (over all Y ; the powers of F need not be uniform). Theorem F is ample iff for all Y and d, H1(FFY , F⊗n(d)) = 0 for n ≫ 0. Theorem F is ample iff its slopes are everywhere positive. Consequently, this condition is pointwise and open on |X|.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 31 / 36

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SLIDE 97

Sheaves on relative Fargues-Fontaine curves

Ampleness for vector bundles

A vector bundle F on FFX is ample if for any vector bundle G on FFY , G ⊗ F⊗n is generated by global sections for n ≫ 0. Theorem O(1) is ample. Consequently, to check ampleness we need only consider G = O(d) for d ∈ Z (over all Y ; the powers of F need not be uniform). Theorem F is ample iff for all Y and d, H1(FFY , F⊗n(d)) = 0 for n ≫ 0. Theorem F is ample iff its slopes are everywhere positive. Consequently, this condition is pointwise and open on |X|.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 31 / 36

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SLIDE 98

Sheaves on relative Fargues-Fontaine curves

Ampleness for vector bundles

A vector bundle F on FFX is ample if for any vector bundle G on FFY , G ⊗ F⊗n is generated by global sections for n ≫ 0. Theorem O(1) is ample. Consequently, to check ampleness we need only consider G = O(d) for d ∈ Z (over all Y ; the powers of F need not be uniform). Theorem F is ample iff for all Y and d, H1(FFY , F⊗n(d)) = 0 for n ≫ 0. Theorem F is ample iff its slopes are everywhere positive. Consequently, this condition is pointwise and open on |X|.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 31 / 36

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SLIDE 99

Sheaves on relative Fargues-Fontaine curves

A distinguished section

So far, FFX has been defined entirely in terms of X ♭ (as in the lecture of Fargues). But it does admit some structures that depend on X: a distinguished ample line bundle LX of rank 1 and degree 1; a distinguished section tX of LX. The zero locus of tX is the image of a section X → FFX of the map |FFX| → |X|. Unlike the fiber map, though, this is a map of adic spaces. It should be possible to define sheaves BdR, Bcrys, Bst; for instance, BdR,X =

  • OFFX [t−1

X ]

where the hat denotes (tX)-adic completion.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 32 / 36

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SLIDE 100

Sheaves on relative Fargues-Fontaine curves

A distinguished section

So far, FFX has been defined entirely in terms of X ♭ (as in the lecture of Fargues). But it does admit some structures that depend on X: a distinguished ample line bundle LX of rank 1 and degree 1; a distinguished section tX of LX. The zero locus of tX is the image of a section X → FFX of the map |FFX| → |X|. Unlike the fiber map, though, this is a map of adic spaces. It should be possible to define sheaves BdR, Bcrys, Bst; for instance, BdR,X =

  • OFFX [t−1

X ]

where the hat denotes (tX)-adic completion.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 32 / 36

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SLIDE 101

The next frontier: imperfect period rings (and maybe sheaves)

Contents

1

Overview: goals of relative p-adic Hodge theory

2

Period sheaves I: Witt vectors and Zp-local systems

3

Period sheaves II: Robba rings and Qp-local systems

4

Sheaves on relative Fargues-Fontaine curves

5

The next frontier: imperfect period rings (and maybe sheaves)

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 33 / 36

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SLIDE 102

The next frontier: imperfect period rings (and maybe sheaves)

The field of norms correspondence

Let K be a p-adic field. Let K∞ be a strictly arithmetically profinite (i.e., “sufficiently infinitely ramified”) algebraic extension of K. The Fontaine-Wintenberger field of norms is a local field L of characteristic p such that K∞

♭ =

  • Lperf. In particular, L is imperfect.

Example: for K = Qp, K∞ = Qp(µp∞), we get L = Fp((π)). Tilting does not find L inside

  • Lperf. The problem is that one must

remember not just K∞ but also K∞, and especially the tower of extensions leading to K∞ via the ramification filtration. Questions: can one similarly “deperfect” the other period rings? And what about other naturally arising perfectoid towers, e.g., the Lubin-Tate tower?

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 34 / 36

slide-103
SLIDE 103

The next frontier: imperfect period rings (and maybe sheaves)

The field of norms correspondence

Let K be a p-adic field. Let K∞ be a strictly arithmetically profinite (i.e., “sufficiently infinitely ramified”) algebraic extension of K. The Fontaine-Wintenberger field of norms is a local field L of characteristic p such that K∞

♭ =

  • Lperf. In particular, L is imperfect.

Example: for K = Qp, K∞ = Qp(µp∞), we get L = Fp((π)). Tilting does not find L inside

  • Lperf. The problem is that one must

remember not just K∞ but also K∞, and especially the tower of extensions leading to K∞ via the ramification filtration. Questions: can one similarly “deperfect” the other period rings? And what about other naturally arising perfectoid towers, e.g., the Lubin-Tate tower?

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 34 / 36

slide-104
SLIDE 104

The next frontier: imperfect period rings (and maybe sheaves)

The field of norms correspondence

Let K be a p-adic field. Let K∞ be a strictly arithmetically profinite (i.e., “sufficiently infinitely ramified”) algebraic extension of K. The Fontaine-Wintenberger field of norms is a local field L of characteristic p such that K∞

♭ =

  • Lperf. In particular, L is imperfect.

Example: for K = Qp, K∞ = Qp(µp∞), we get L = Fp((π)). Tilting does not find L inside

  • Lperf. The problem is that one must

remember not just K∞ but also K∞, and especially the tower of extensions leading to K∞ via the ramification filtration. Questions: can one similarly “deperfect” the other period rings? And what about other naturally arising perfectoid towers, e.g., the Lubin-Tate tower?

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 34 / 36

slide-105
SLIDE 105

The next frontier: imperfect period rings (and maybe sheaves)

The field of norms correspondence

Let K be a p-adic field. Let K∞ be a strictly arithmetically profinite (i.e., “sufficiently infinitely ramified”) algebraic extension of K. The Fontaine-Wintenberger field of norms is a local field L of characteristic p such that K∞

♭ =

  • Lperf. In particular, L is imperfect.

Example: for K = Qp, K∞ = Qp(µp∞), we get L = Fp((π)). Tilting does not find L inside

  • Lperf. The problem is that one must

remember not just K∞ but also K∞, and especially the tower of extensions leading to K∞ via the ramification filtration. Questions: can one similarly “deperfect” the other period rings? And what about other naturally arising perfectoid towers, e.g., the Lubin-Tate tower?

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 34 / 36

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SLIDE 106

The next frontier: imperfect period rings (and maybe sheaves)

The example of (ϕ, Γ)-modules

For K = Qp, K∞ = Qp(µp∞), map A = lim ← −n→∞(Z/pnZ)((π)) into ˜ A = ˜ A

K∞ by taking 1 + π to [1 + π]. Then Γ lifts to A and A†.

Theorem (Cherbonnier-Colmez) The categories of (ϕ, Γ)-modules (ϕ-modules with compatible Γ-action)

  • ver A, A†, ˜

A, ˜ A† are all equivalent. Consequently, elements of RepQp(GK) define ϕ-modules over the Robba ring C. By taking sections over annuli, we get locally analytic representations of Γ; this doesn’t happen using ϕ-modules over ˜ C.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 35 / 36

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SLIDE 107

The next frontier: imperfect period rings (and maybe sheaves)

The example of (ϕ, Γ)-modules

For K = Qp, K∞ = Qp(µp∞), map A = lim ← −n→∞(Z/pnZ)((π)) into ˜ A = ˜ A

K∞ by taking 1 + π to [1 + π]. Then Γ lifts to A and A†.

Theorem (Cherbonnier-Colmez) The categories of (ϕ, Γ)-modules (ϕ-modules with compatible Γ-action)

  • ver A, A†, ˜

A, ˜ A† are all equivalent. Consequently, elements of RepQp(GK) define ϕ-modules over the Robba ring C. By taking sections over annuli, we get locally analytic representations of Γ; this doesn’t happen using ϕ-modules over ˜ C.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 35 / 36

slide-108
SLIDE 108

The next frontier: imperfect period rings (and maybe sheaves)

The example of (ϕ, Γ)-modules

For K = Qp, K∞ = Qp(µp∞), map A = lim ← −n→∞(Z/pnZ)((π)) into ˜ A = ˜ A

K∞ by taking 1 + π to [1 + π]. Then Γ lifts to A and A†.

Theorem (Cherbonnier-Colmez) The categories of (ϕ, Γ)-modules (ϕ-modules with compatible Γ-action)

  • ver A, A†, ˜

A, ˜ A† are all equivalent. Consequently, elements of RepQp(GK) define ϕ-modules over the Robba ring C. By taking sections over annuli, we get locally analytic representations of Γ; this doesn’t happen using ϕ-modules over ˜ C.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 35 / 36

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SLIDE 109

The next frontier: imperfect period rings (and maybe sheaves)

Relative Cherbonnier-Colmez

One may hope for an analogue of Cherbonnier-Colmez for other perfectoid towers, i.e., descent of ϕ-modules with descent data from ˜ A to some appropriate imperfect subring A. This would perhaps give additional locally analytic representations sought by Berger-Colmez. (One may also want to descent from ˜ C to a suitable C.) One well-understood case are towers arising from the standard perfectoid tower over Pn (Andreatta-Brinon); these towers are used in the p-adic comparison isomorphism (see Nizio l’s lectures). Important question: what about the Lubin-Tate tower (see Weinstein’s lectures)? And (how) is this relevant to p-adic Langlands? See the next version of “Relative p-adic Hodge theory, II”.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 36 / 36

slide-110
SLIDE 110

The next frontier: imperfect period rings (and maybe sheaves)

Relative Cherbonnier-Colmez

One may hope for an analogue of Cherbonnier-Colmez for other perfectoid towers, i.e., descent of ϕ-modules with descent data from ˜ A to some appropriate imperfect subring A. This would perhaps give additional locally analytic representations sought by Berger-Colmez. (One may also want to descent from ˜ C to a suitable C.) One well-understood case are towers arising from the standard perfectoid tower over Pn (Andreatta-Brinon); these towers are used in the p-adic comparison isomorphism (see Nizio l’s lectures). Important question: what about the Lubin-Tate tower (see Weinstein’s lectures)? And (how) is this relevant to p-adic Langlands? See the next version of “Relative p-adic Hodge theory, II”.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 36 / 36

slide-111
SLIDE 111

The next frontier: imperfect period rings (and maybe sheaves)

Relative Cherbonnier-Colmez

One may hope for an analogue of Cherbonnier-Colmez for other perfectoid towers, i.e., descent of ϕ-modules with descent data from ˜ A to some appropriate imperfect subring A. This would perhaps give additional locally analytic representations sought by Berger-Colmez. (One may also want to descent from ˜ C to a suitable C.) One well-understood case are towers arising from the standard perfectoid tower over Pn (Andreatta-Brinon); these towers are used in the p-adic comparison isomorphism (see Nizio l’s lectures). Important question: what about the Lubin-Tate tower (see Weinstein’s lectures)? And (how) is this relevant to p-adic Langlands? See the next version of “Relative p-adic Hodge theory, II”.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 36 / 36

slide-112
SLIDE 112

The next frontier: imperfect period rings (and maybe sheaves)

Relative Cherbonnier-Colmez

One may hope for an analogue of Cherbonnier-Colmez for other perfectoid towers, i.e., descent of ϕ-modules with descent data from ˜ A to some appropriate imperfect subring A. This would perhaps give additional locally analytic representations sought by Berger-Colmez. (One may also want to descent from ˜ C to a suitable C.) One well-understood case are towers arising from the standard perfectoid tower over Pn (Andreatta-Brinon); these towers are used in the p-adic comparison isomorphism (see Nizio l’s lectures). Important question: what about the Lubin-Tate tower (see Weinstein’s lectures)? And (how) is this relevant to p-adic Langlands? See the next version of “Relative p-adic Hodge theory, II”.

Kiran S. Kedlaya (UCSD) Relative p-adic Hodge theory 36 / 36