Non-archimedean Dynamics in Dimension One: Lecture...

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Non-archimedean Dynamics in Dimension One: Lecture 2 Robert L. Benedetto Amherst College Arizona Winter School Sunday, March 14, 2010

Transcript of Non-archimedean Dynamics in Dimension One: Lecture...

Page 1: Non-archimedean Dynamics in Dimension One: Lecture 2swc.math.arizona.edu/aws/2010/2010BenedettoLectureNotes2.pdf · There are ways to get around that (see Section 5 of the lecture

Non-archimedean Dynamics in Dimension One:Lecture 2

Robert L. BenedettoAmherst College

Arizona Winter School

Sunday, March 14, 2010

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Problems with P1(CK )

◮ P1(CK ) is not compact, or even locally compact.

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Problems with P1(CK )

◮ P1(CK ) is not compact, or even locally compact.

◮ P1(CK ) is totally disconnected.

That makes it hard to study “components” of the Fatou setin a meaningful way.

Page 4: Non-archimedean Dynamics in Dimension One: Lecture 2swc.math.arizona.edu/aws/2010/2010BenedettoLectureNotes2.pdf · There are ways to get around that (see Section 5 of the lecture

Problems with P1(CK )

◮ P1(CK ) is not compact, or even locally compact.

◮ P1(CK ) is totally disconnected.

That makes it hard to study “components” of the Fatou setin a meaningful way.

There are ways to get around that (see Section 5 of thelecture notes), but there is a better way.

Page 5: Non-archimedean Dynamics in Dimension One: Lecture 2swc.math.arizona.edu/aws/2010/2010BenedettoLectureNotes2.pdf · There are ways to get around that (see Section 5 of the lecture

Problems with P1(CK )

◮ P1(CK ) is not compact, or even locally compact.

◮ P1(CK ) is totally disconnected.

That makes it hard to study “components” of the Fatou setin a meaningful way.

There are ways to get around that (see Section 5 of thelecture notes), but there is a better way.

There is a nicer space P1Ber that:

◮ contains P1(CK ) as a subspace,

Page 6: Non-archimedean Dynamics in Dimension One: Lecture 2swc.math.arizona.edu/aws/2010/2010BenedettoLectureNotes2.pdf · There are ways to get around that (see Section 5 of the lecture

Problems with P1(CK )

◮ P1(CK ) is not compact, or even locally compact.

◮ P1(CK ) is totally disconnected.

That makes it hard to study “components” of the Fatou setin a meaningful way.

There are ways to get around that (see Section 5 of thelecture notes), but there is a better way.

There is a nicer space P1Ber that:

◮ contains P1(CK ) as a subspace,

◮ is compact,

Page 7: Non-archimedean Dynamics in Dimension One: Lecture 2swc.math.arizona.edu/aws/2010/2010BenedettoLectureNotes2.pdf · There are ways to get around that (see Section 5 of the lecture

Problems with P1(CK )

◮ P1(CK ) is not compact, or even locally compact.

◮ P1(CK ) is totally disconnected.

That makes it hard to study “components” of the Fatou setin a meaningful way.

There are ways to get around that (see Section 5 of thelecture notes), but there is a better way.

There is a nicer space P1Ber that:

◮ contains P1(CK ) as a subspace,

◮ is compact,

◮ is (still) Hausdorff, and

Page 8: Non-archimedean Dynamics in Dimension One: Lecture 2swc.math.arizona.edu/aws/2010/2010BenedettoLectureNotes2.pdf · There are ways to get around that (see Section 5 of the lecture

Problems with P1(CK )

◮ P1(CK ) is not compact, or even locally compact.

◮ P1(CK ) is totally disconnected.

That makes it hard to study “components” of the Fatou setin a meaningful way.

There are ways to get around that (see Section 5 of thelecture notes), but there is a better way.

There is a nicer space P1Ber that:

◮ contains P1(CK ) as a subspace,

◮ is compact,

◮ is (still) Hausdorff, and

◮ is path-connected.

Page 9: Non-archimedean Dynamics in Dimension One: Lecture 2swc.math.arizona.edu/aws/2010/2010BenedettoLectureNotes2.pdf · There are ways to get around that (see Section 5 of the lecture

The Gauss NormA(0, 1) = CK 〈〈z〉〉 is the ring of all power series

f (z) =∞

n=0

cnzn ∈ CK [[z ]] such that lim

n→∞cn = 0,

i.e., the ring of power series converging on D(0, 1).

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The Gauss NormA(0, 1) = CK 〈〈z〉〉 is the ring of all power series

f (z) =∞

n=0

cnzn ∈ CK [[z ]] such that lim

n→∞cn = 0,

i.e., the ring of power series converging on D(0, 1).

The Gauss norm on A(0, 1) is ‖ · ‖ζ(0,1) : A(0, 1) → [0,∞), by

∞∑

n=0

cnzn∥

ζ(0,1):= max{|cn| : n ≥ 0}.

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The Gauss NormA(0, 1) = CK 〈〈z〉〉 is the ring of all power series

f (z) =∞

n=0

cnzn ∈ CK [[z ]] such that lim

n→∞cn = 0,

i.e., the ring of power series converging on D(0, 1).

The Gauss norm on A(0, 1) is ‖ · ‖ζ(0,1) : A(0, 1) → [0,∞), by

∞∑

n=0

cnzn∥

ζ(0,1):= max{|cn| : n ≥ 0}.

Equivalently, for all f ∈ A(0, 1),

‖f ‖ζ(0,1) := sup{|f (x)| : x ∈ D(0, 1)}

= max{|f (x)| : x ∈ D(0, 1)}

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Bounded Multiplicative Seminorms

DefinitionA bounded multiplicative seminorm on A(0, 1) is a functionζ = ‖ · ‖ζ : A(0, 1) → [0,∞) such that

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Bounded Multiplicative Seminorms

DefinitionA bounded multiplicative seminorm on A(0, 1) is a functionζ = ‖ · ‖ζ : A(0, 1) → [0,∞) such that

◮ ‖0‖ζ = 0 and ‖1‖ζ = 1,

◮ ‖fg‖ζ = ‖f ‖ζ · ‖g‖ζ for all f , g ∈ A(0, 1),

◮ ‖f + g‖ζ ≤ ‖f ‖ζ + ‖g‖ζ for all f , g ∈ A(0, 1), and

◮ ‖f ‖ζ ≤ ‖f ‖ζ(0,1) for all f ∈ A(0, 1).

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Bounded Multiplicative Seminorms

DefinitionA bounded multiplicative seminorm on A(0, 1) is a functionζ = ‖ · ‖ζ : A(0, 1) → [0,∞) such that

◮ ‖0‖ζ = 0 and ‖1‖ζ = 1,

◮ ‖fg‖ζ = ‖f ‖ζ · ‖g‖ζ for all f , g ∈ A(0, 1),

◮ ‖f + g‖ζ ≤ ‖f ‖ζ + ‖g‖ζ for all f , g ∈ A(0, 1), and

◮ ‖f ‖ζ ≤ ‖f ‖ζ(0,1) for all f ∈ A(0, 1).

Note: We do not require that ‖f ‖ζ = 0 implies f = 0.

Page 15: Non-archimedean Dynamics in Dimension One: Lecture 2swc.math.arizona.edu/aws/2010/2010BenedettoLectureNotes2.pdf · There are ways to get around that (see Section 5 of the lecture

Bounded Multiplicative Seminorms

DefinitionA bounded multiplicative seminorm on A(0, 1) is a functionζ = ‖ · ‖ζ : A(0, 1) → [0,∞) such that

◮ ‖0‖ζ = 0 and ‖1‖ζ = 1,

◮ ‖fg‖ζ = ‖f ‖ζ · ‖g‖ζ for all f , g ∈ A(0, 1),

◮ ‖f + g‖ζ ≤ ‖f ‖ζ + ‖g‖ζ for all f , g ∈ A(0, 1), and

◮ ‖f ‖ζ ≤ ‖f ‖ζ(0,1) for all f ∈ A(0, 1).

Note: We do not require that ‖f ‖ζ = 0 implies f = 0.

By the way: we get ‖f + g‖ζ ≤ max{‖f ‖ζ , ‖g‖ζ} for free.

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Examples of Bounded Multiplicative Seminorms

1. For any x ∈ D(0, 1), define ‖ · ‖x by ‖f ‖x := |f (x)|.

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Examples of Bounded Multiplicative Seminorms

1. For any x ∈ D(0, 1), define ‖ · ‖x by ‖f ‖x := |f (x)|.

2. For any disk D ⊆ D(0, 1), define ‖ · ‖D by

‖f ‖D := sup{|f (x)| : x ∈ D}.

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Examples of Bounded Multiplicative Seminorms

1. For any x ∈ D(0, 1), define ‖ · ‖x by ‖f ‖x := |f (x)|.

2. For any disk D ⊆ D(0, 1), define ‖ · ‖D by

‖f ‖D := sup{|f (x)| : x ∈ D}.

If D = D(a, r) or D = D(a, r), and f (z) =∑

cn(z − a)n, then

‖f ‖D = max{|cn|rn : n ≥ 0}.

If D is rational closed, then ‖f ‖D = max{|f (x)| : x ∈ D}.

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Examples of Bounded Multiplicative Seminorms

1. For any x ∈ D(0, 1), define ‖ · ‖x by ‖f ‖x := |f (x)|.

2. For any disk D ⊆ D(0, 1), define ‖ · ‖D by

‖f ‖D := sup{|f (x)| : x ∈ D}.

If D = D(a, r) or D = D(a, r), and f (z) =∑

cn(z − a)n, then

‖f ‖D = max{|cn|rn : n ≥ 0}.

If D is rational closed, then ‖f ‖D = max{|f (x)| : x ∈ D}.

Since ‖ · ‖D(a,r) = ‖ · ‖D(a,r), we can denote both by ‖ · ‖ζ(a,r).

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The Berkovich Disk

DefinitionThe Berkovich unit disk DBer(0, 1) is the set of all boundedmultiplicative seminorms on A(0, 1).

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The Berkovich Disk

DefinitionThe Berkovich unit disk DBer(0, 1) is the set of all boundedmultiplicative seminorms on A(0, 1).

As a topological space, DBer(0, 1) is equipped with the Gel’fandtopology.

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The Berkovich Disk

DefinitionThe Berkovich unit disk DBer(0, 1) is the set of all boundedmultiplicative seminorms on A(0, 1).

As a topological space, DBer(0, 1) is equipped with the Gel’fandtopology.

This is the weakest topology such that for every f ∈ A(0, 1), themap DBer(0, 1) → R given by

ζ 7→ ‖f ‖ζ

is continuous.

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Berkovich’s Classification of Points

There are four kinds of points in DBer(0, 1).

1. Type I: seminorms ‖ · ‖x corresponding to (classical) pointsx ∈ D(0, 1).

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Berkovich’s Classification of Points

There are four kinds of points in DBer(0, 1).

1. Type I: seminorms ‖ · ‖x corresponding to (classical) pointsx ∈ D(0, 1).

2. Type II: norms ‖ · ‖ζ(a,r) corresponding to rational closed

disks D(a, r) ⊆ D(0, 1).

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Berkovich’s Classification of Points

There are four kinds of points in DBer(0, 1).

1. Type I: seminorms ‖ · ‖x corresponding to (classical) pointsx ∈ D(0, 1).

2. Type II: norms ‖ · ‖ζ(a,r) corresponding to rational closed

disks D(a, r) ⊆ D(0, 1).

3. Type III: norms ‖ · ‖ζ(a,r) corresponding to irrational disks

D(a, r) ⊂ D(0, 1).

Page 26: Non-archimedean Dynamics in Dimension One: Lecture 2swc.math.arizona.edu/aws/2010/2010BenedettoLectureNotes2.pdf · There are ways to get around that (see Section 5 of the lecture

Berkovich’s Classification of Points

There are four kinds of points in DBer(0, 1).

1. Type I: seminorms ‖ · ‖x corresponding to (classical) pointsx ∈ D(0, 1).

2. Type II: norms ‖ · ‖ζ(a,r) corresponding to rational closed

disks D(a, r) ⊆ D(0, 1).

3. Type III: norms ‖ · ‖ζ(a,r) corresponding to irrational disks

D(a, r) ⊂ D(0, 1).

4. Type IV: norms ‖ · ‖ζ corresponding to (equivalence classesof) decreasing chains D1 ⊇ D2 ⊇ · · · of disks with emptyintersection.

Chains of disks as in Type IV must have radius bounded below.

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Path-connectedness, intuitively

x

y

D(0,1)

D(x,|x-y|)=D(y,|x-y|)

D(x,r)

D(y,r)

x y

ζ(x,r) ζ(y,r)

ζ(x,|x-y|)

ζ(0,1)

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DBer(0, 1) as an R-tree

ζ(0,1)

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The Berkovich Projective Line P1Ber

Glue two copies of DBer(0, 1) along |z | = 1 via z 7→ 1/z .

0

1

α

ζ(0,1)

ζ(0,|α|)=ζ(α,|α|)

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Berkovich Disks

DefinitionLet a ∈ CK and r > 0.

◮ The closed Berkovich disk DBer(a, r) is the set of allζ ∈ P

1Ber corresponding to a point/disk/chain of disks

contained in D(a, r).

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Berkovich Disks

DefinitionLet a ∈ CK and r > 0.

◮ The closed Berkovich disk DBer(a, r) is the set of allζ ∈ P

1Ber corresponding to a point/disk/chain of disks

contained in D(a, r).

◮ The open Berkovich disk DBer(a, r) is the set of all ζ ∈ P1Ber

corresponding to a point/disk/chain of disks contained inD(a, r), except ζ(a, r) itself.

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Berkovich Disks

DefinitionLet a ∈ CK and r > 0.

◮ The closed Berkovich disk DBer(a, r) is the set of allζ ∈ P

1Ber corresponding to a point/disk/chain of disks

contained in D(a, r).

◮ The open Berkovich disk DBer(a, r) is the set of all ζ ∈ P1Ber

corresponding to a point/disk/chain of disks contained inD(a, r), except ζ(a, r) itself.

Fact:

DBer(a, r) is open, and DBer(a, r) is closed.

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Berkovich Disks

DefinitionLet a ∈ CK and r > 0.

◮ The closed Berkovich disk DBer(a, r) is the set of allζ ∈ P

1Ber corresponding to a point/disk/chain of disks

contained in D(a, r).

◮ The open Berkovich disk DBer(a, r) is the set of all ζ ∈ P1Ber

corresponding to a point/disk/chain of disks contained inD(a, r), except ζ(a, r) itself.

Fact:

DBer(a, r) is open, and DBer(a, r) is closed.

Moreover:The open Berkovich disks and the complements of closedBerkovich disks together form a subbasis for the Gel’fand topology.

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More on the Gel’fand Topology

DefinitionAn (open) connected Berkovich affinoid is the intersection offinitely many (open) Berkovich disks and complements of (closed)Berkovich disks.

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More on the Gel’fand Topology

DefinitionAn (open) connected Berkovich affinoid is the intersection offinitely many (open) Berkovich disks and complements of (closed)Berkovich disks.

Theorem

◮ The open connected Berkovich affinoids form a basis for the

Gel’fand topology.

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More on the Gel’fand Topology

DefinitionAn (open) connected Berkovich affinoid is the intersection offinitely many (open) Berkovich disks and complements of (closed)Berkovich disks.

Theorem

◮ The open connected Berkovich affinoids form a basis for the

Gel’fand topology.

◮ P1Ber is uniquely path-connected.

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More on the Gel’fand Topology

DefinitionAn (open) connected Berkovich affinoid is the intersection offinitely many (open) Berkovich disks and complements of (closed)Berkovich disks.

Theorem

◮ The open connected Berkovich affinoids form a basis for the

Gel’fand topology.

◮ P1Ber is uniquely path-connected.

For any ζ ∈ P1Ber, the complement P1

Ber r {ζ} consists of

1. one component if ζ is type I or type IV,

2. infinitely many components if ζ is type II,

3. two components if ζ is type III.

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More on the Gel’fand Topology

DefinitionAn (open) connected Berkovich affinoid is the intersection offinitely many (open) Berkovich disks and complements of (closed)Berkovich disks.

Theorem

◮ The open connected Berkovich affinoids form a basis for the

Gel’fand topology.

◮ P1Ber is uniquely path-connected.

For any ζ ∈ P1Ber, the complement P1

Ber r {ζ} consists of

1. one component if ζ is type I or type IV,

2. infinitely many components if ζ is type II,

3. two components if ζ is type III.

The components of P1Ber r {ζ} are called the directions at ζ.

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Recall: The Berkovich Projective Line P1Ber

0

1

α

ζ(0,1)

ζ(0,|α|)=ζ(α,|α|)

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Rational Functions Acting on P1Ber

Let φ(z) ∈ CK (z). Then for each point ζ ∈ P1Ber, there is a unique

point φ(ζ) ∈ P1Ber such that

‖h‖φ(ζ) = ‖φ ◦ h‖ζ

for all h ∈ CK (z).

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Rational Functions Acting on P1Ber

Let φ(z) ∈ CK (z). Then for each point ζ ∈ P1Ber, there is a unique

point φ(ζ) ∈ P1Ber such that

‖h‖φ(ζ) = ‖φ ◦ h‖ζ

for all h ∈ CK (z).

If ζ is type I, then φ(ζ) is what you think.

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Rational Functions Acting on P1Ber

Let φ(z) ∈ CK (z). Then for each point ζ ∈ P1Ber, there is a unique

point φ(ζ) ∈ P1Ber such that

‖h‖φ(ζ) = ‖φ ◦ h‖ζ

for all h ∈ CK (z).

If ζ is type I, then φ(ζ) is what you think.

Then φ : P1Ber → P1

Ber is the unique continuous extension ofφ : P

1(CK ) → P1(CK ).

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Understanding degree one maps on P1Ber

◮ φ(z) = cz maps ζ(a, r) to ζ(ca, |c |r).

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Understanding degree one maps on P1Ber

◮ φ(z) = cz maps ζ(a, r) to ζ(ca, |c |r).

◮ φ(z) = z + b maps ζ(a, r) to ζ(a + b, r).

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Understanding degree one maps on P1Ber

◮ φ(z) = cz maps ζ(a, r) to ζ(ca, |c |r).

◮ φ(z) = z + b maps ζ(a, r) to ζ(a + b, r).

◮ φ(z) = 1/z maps ζ(a, r) to

{

ζ(0, 1/r) if 0 ∈ D(a, r),

ζ(1/a, r/|a|2) if 0 6∈ D(a, r).

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Understanding degree one maps on P1Ber

◮ φ(z) = cz maps ζ(a, r) to ζ(ca, |c |r).

◮ φ(z) = z + b maps ζ(a, r) to ζ(a + b, r).

◮ φ(z) = 1/z maps ζ(a, r) to

{

ζ(0, 1/r) if 0 ∈ D(a, r),

ζ(1/a, r/|a|2) if 0 6∈ D(a, r).

◮ So for any φ ∈ PGL(2, CK ), i.e., φ(z) =az + b

cz + dwith

ad − bc 6= 0, you can figure out what φ(ζ) is for any ζ ∈ P1Ber.

Page 47: Non-archimedean Dynamics in Dimension One: Lecture 2swc.math.arizona.edu/aws/2010/2010BenedettoLectureNotes2.pdf · There are ways to get around that (see Section 5 of the lecture

Understanding degree one maps on P1Ber

◮ φ(z) = cz maps ζ(a, r) to ζ(ca, |c |r).

◮ φ(z) = z + b maps ζ(a, r) to ζ(a + b, r).

◮ φ(z) = 1/z maps ζ(a, r) to

{

ζ(0, 1/r) if 0 ∈ D(a, r),

ζ(1/a, r/|a|2) if 0 6∈ D(a, r).

◮ So for any φ ∈ PGL(2, CK ), i.e., φ(z) =az + b

cz + dwith

ad − bc 6= 0, you can figure out what φ(ζ) is for any ζ ∈ P1Ber.

◮ Given φ ∈ PGL(2, CK ), then

φ(ζ(0, 1)) = ζ(0, 1) if and only if φ ∈ PGL(2,O),

Page 48: Non-archimedean Dynamics in Dimension One: Lecture 2swc.math.arizona.edu/aws/2010/2010BenedettoLectureNotes2.pdf · There are ways to get around that (see Section 5 of the lecture

Understanding degree one maps on P1Ber

◮ φ(z) = cz maps ζ(a, r) to ζ(ca, |c |r).

◮ φ(z) = z + b maps ζ(a, r) to ζ(a + b, r).

◮ φ(z) = 1/z maps ζ(a, r) to

{

ζ(0, 1/r) if 0 ∈ D(a, r),

ζ(1/a, r/|a|2) if 0 6∈ D(a, r).

◮ So for any φ ∈ PGL(2, CK ), i.e., φ(z) =az + b

cz + dwith

ad − bc 6= 0, you can figure out what φ(ζ) is for any ζ ∈ P1Ber.

◮ Given φ ∈ PGL(2, CK ), then

φ(ζ(0, 1)) = ζ(0, 1) if and only if φ ∈ PGL(2,O),

i.e., φ(z) =az + b

cz + dwith |a|, |b|, |c |, |d | ≤ 1 and |ad −bc | = 1.

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Reduction of φ ∈ CK (z)

For more general φ ∈ CK (z), when does φ(ζ(0, 1)) = ζ(0, 1)?

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Reduction of φ ∈ CK (z)

For more general φ ∈ CK (z), when does φ(ζ(0, 1)) = ζ(0, 1)?

Write φ(z) =adzd + · · · + a1z + a0

bdzd + · · · + b1z + b0,

with ai , bi ∈ O and some |ai | = 1 and/or some |bj | = 1.

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Reduction of φ ∈ CK (z)

For more general φ ∈ CK (z), when does φ(ζ(0, 1)) = ζ(0, 1)?

Write φ(z) =adzd + · · · + a1z + a0

bdzd + · · · + b1z + b0,

with ai , bi ∈ O and some |ai | = 1 and/or some |bj | = 1.

Then φ(z) :=adzd + · · · + a1z + a0

bdzd + · · · + b1z + b0

∈ k(z).

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Reduction of φ ∈ CK (z)

For more general φ ∈ CK (z), when does φ(ζ(0, 1)) = ζ(0, 1)?

Write φ(z) =adzd + · · · + a1z + a0

bdzd + · · · + b1z + b0,

with ai , bi ∈ O and some |ai | = 1 and/or some |bj | = 1.

Then φ(z) :=adzd + · · · + a1z + a0

bdzd + · · · + b1z + b0

∈ k(z).

But we might have cancellation in φ.

Page 53: Non-archimedean Dynamics in Dimension One: Lecture 2swc.math.arizona.edu/aws/2010/2010BenedettoLectureNotes2.pdf · There are ways to get around that (see Section 5 of the lecture

Reduction of φ ∈ CK (z)

For more general φ ∈ CK (z), when does φ(ζ(0, 1)) = ζ(0, 1)?

Write φ(z) =adzd + · · · + a1z + a0

bdzd + · · · + b1z + b0,

with ai , bi ∈ O and some |ai | = 1 and/or some |bj | = 1.

Then φ(z) :=adzd + · · · + a1z + a0

bdzd + · · · + b1z + b0

∈ k(z).

But we might have cancellation in φ.

If deg φ = deg φ, we say φ has good reduction.If deg φ ≥ 1, we say φ has nonconstant reduction.

Page 54: Non-archimedean Dynamics in Dimension One: Lecture 2swc.math.arizona.edu/aws/2010/2010BenedettoLectureNotes2.pdf · There are ways to get around that (see Section 5 of the lecture

Reduction of φ ∈ CK (z)

For more general φ ∈ CK (z), when does φ(ζ(0, 1)) = ζ(0, 1)?

Write φ(z) =adzd + · · · + a1z + a0

bdzd + · · · + b1z + b0,

with ai , bi ∈ O and some |ai | = 1 and/or some |bj | = 1.

Then φ(z) :=adzd + · · · + a1z + a0

bdzd + · · · + b1z + b0

∈ k(z).

But we might have cancellation in φ.

If deg φ = deg φ, we say φ has good reduction.If deg φ ≥ 1, we say φ has nonconstant reduction.

Fact: φ(ζ(0, 1)) = ζ(0, 1) if and only if φ has nonconstantreduction.

Page 55: Non-archimedean Dynamics in Dimension One: Lecture 2swc.math.arizona.edu/aws/2010/2010BenedettoLectureNotes2.pdf · There are ways to get around that (see Section 5 of the lecture

Understanding φ ∈ CK (z) at type II points

◮ For any type II point ζ ∈ P1Ber, there is some η ∈ PGL(2, CK )

such that η(ζ) = ζ(0, 1).

Page 56: Non-archimedean Dynamics in Dimension One: Lecture 2swc.math.arizona.edu/aws/2010/2010BenedettoLectureNotes2.pdf · There are ways to get around that (see Section 5 of the lecture

Understanding φ ∈ CK (z) at type II points

◮ For any type II point ζ ∈ P1Ber, there is some η ∈ PGL(2, CK )

such that η(ζ) = ζ(0, 1).

◮ Given φ ∈ CK (z) nonconstant and ζ ∈ P1Ber of type II, choose

η ∈ PGL(2, CK ) for ζ as above.

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Understanding φ ∈ CK (z) at type II points

◮ For any type II point ζ ∈ P1Ber, there is some η ∈ PGL(2, CK )

such that η(ζ) = ζ(0, 1).

◮ Given φ ∈ CK (z) nonconstant and ζ ∈ P1Ber of type II, choose

η ∈ PGL(2, CK ) for ζ as above. Then there is someθ ∈ PGL(2, CK ) such that the rational function

θ ◦ φ ◦ η−1(z) ∈ CK (z)

has nonconstant reduction.

Page 58: Non-archimedean Dynamics in Dimension One: Lecture 2swc.math.arizona.edu/aws/2010/2010BenedettoLectureNotes2.pdf · There are ways to get around that (see Section 5 of the lecture

Understanding φ ∈ CK (z) at type II points

◮ For any type II point ζ ∈ P1Ber, there is some η ∈ PGL(2, CK )

such that η(ζ) = ζ(0, 1).

◮ Given φ ∈ CK (z) nonconstant and ζ ∈ P1Ber of type II, choose

η ∈ PGL(2, CK ) for ζ as above. Then there is someθ ∈ PGL(2, CK ) such that the rational function

θ ◦ φ ◦ η−1(z) ∈ CK (z)

has nonconstant reduction.

◮ Then φ(ζ) = θ−1(ζ(0, 1)).

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Understanding φ ∈ CK (z) at type II points

◮ For any type II point ζ ∈ P1Ber, there is some η ∈ PGL(2, CK )

such that η(ζ) = ζ(0, 1).

◮ Given φ ∈ CK (z) nonconstant and ζ ∈ P1Ber of type II, choose

η ∈ PGL(2, CK ) for ζ as above. Then there is someθ ∈ PGL(2, CK ) such that the rational function

θ ◦ φ ◦ η−1(z) ∈ CK (z)

has nonconstant reduction.

◮ Then φ(ζ) = θ−1(ζ(0, 1)).

◮ η, θ ∈ PGL(2, CK ) are not unique,but the cosets PGL(2,O)η and PGL(2,O)θ are unique.

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Example

CK = Cp, ζ = ζ(0, |p|p), and φ(z) =z3 − z2 + z + p2

z.

What is φ(ζ)?

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Example

CK = Cp, ζ = ζ(0, |p|p), and φ(z) =z3 − z2 + z + p2

z.

What is φ(ζ)?

η(z) = z/p maps ζ to ζ(0, 1), and

φ ◦ η−1(z) = φ(pz) =p2z3 − pz2 + z + p

z.

Note φ ◦ η−1 = z/z = 1 is constant.

Page 62: Non-archimedean Dynamics in Dimension One: Lecture 2swc.math.arizona.edu/aws/2010/2010BenedettoLectureNotes2.pdf · There are ways to get around that (see Section 5 of the lecture

Example

CK = Cp, ζ = ζ(0, |p|p), and φ(z) =z3 − z2 + z + p2

z.

What is φ(ζ)?

η(z) = z/p maps ζ to ζ(0, 1), and

φ ◦ η−1(z) = φ(pz) =p2z3 − pz2 + z + p

z.

Note φ ◦ η−1 = z/z = 1 is constant.

So let θ(z) = (z − 1)/p.

Page 63: Non-archimedean Dynamics in Dimension One: Lecture 2swc.math.arizona.edu/aws/2010/2010BenedettoLectureNotes2.pdf · There are ways to get around that (see Section 5 of the lecture

Example

CK = Cp, ζ = ζ(0, |p|p), and φ(z) =z3 − z2 + z + p2

z.

What is φ(ζ)?

η(z) = z/p maps ζ to ζ(0, 1), and

φ ◦ η−1(z) = φ(pz) =p2z3 − pz2 + z + p

z.

Note φ ◦ η−1 = z/z = 1 is constant.

So let θ(z) = (z − 1)/p.

Then θ ◦ φ ◦ η−1(z) =pz3 − z2 + 1

z, and so

θ ◦ φ ◦ η−1(z) = (1 − z2)/z is nonconstant.

Page 64: Non-archimedean Dynamics in Dimension One: Lecture 2swc.math.arizona.edu/aws/2010/2010BenedettoLectureNotes2.pdf · There are ways to get around that (see Section 5 of the lecture

Example

CK = Cp, ζ = ζ(0, |p|p), and φ(z) =z3 − z2 + z + p2

z.

What is φ(ζ)?

η(z) = z/p maps ζ to ζ(0, 1), and

φ ◦ η−1(z) = φ(pz) =p2z3 − pz2 + z + p

z.

Note φ ◦ η−1 = z/z = 1 is constant.

So let θ(z) = (z − 1)/p.

Then θ ◦ φ ◦ η−1(z) =pz3 − z2 + 1

z, and so

θ ◦ φ ◦ η−1(z) = (1 − z2)/z is nonconstant.

So φ(ζ) = θ−1(ζ(0, 1)) = ζ(1, |p|p).

Page 65: Non-archimedean Dynamics in Dimension One: Lecture 2swc.math.arizona.edu/aws/2010/2010BenedettoLectureNotes2.pdf · There are ways to get around that (see Section 5 of the lecture

Dynamics on P1Ber: Classifying Periodic Points

DefinitionIf ζ and ξ are type II points and φ(ζ) = ξ, then the local degreeor multiplicity of φ at ζ is

degζ φ := deg θ ◦ φ ◦ η−1,

where η(ζ) = ζ(0, 1) and θ(ξ) = ζ(0, 1).

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Dynamics on P1Ber: Classifying Periodic Points

DefinitionIf ζ and ξ are type II points and φ(ζ) = ξ, then the local degreeor multiplicity of φ at ζ is

degζ φ := deg θ ◦ φ ◦ η−1,

where η(ζ) = ζ(0, 1) and θ(ξ) = ζ(0, 1).

If ζ is type II and periodic of exact period n, we say ζ is

◮ indifferent (or neutral) if degζ φn = 1.

◮ repelling if degζ φn ≥ 2.

Page 67: Non-archimedean Dynamics in Dimension One: Lecture 2swc.math.arizona.edu/aws/2010/2010BenedettoLectureNotes2.pdf · There are ways to get around that (see Section 5 of the lecture

Dynamics on P1Ber: Classifying Periodic Points

DefinitionIf ζ and ξ are type II points and φ(ζ) = ξ, then the local degreeor multiplicity of φ at ζ is

degζ φ := deg θ ◦ φ ◦ η−1,

where η(ζ) = ζ(0, 1) and θ(ξ) = ζ(0, 1).

If ζ is type II and periodic of exact period n, we say ζ is

◮ indifferent (or neutral) if degζ φn = 1.

◮ repelling if degζ φn ≥ 2.

Warning: Repelling type II points (usually) do not actually repelin most directions.

Page 68: Non-archimedean Dynamics in Dimension One: Lecture 2swc.math.arizona.edu/aws/2010/2010BenedettoLectureNotes2.pdf · There are ways to get around that (see Section 5 of the lecture

Dynamics on P1Ber: Classifying Periodic Points

DefinitionIf ζ and ξ are type II points and φ(ζ) = ξ, then the local degreeor multiplicity of φ at ζ is

degζ φ := deg θ ◦ φ ◦ η−1,

where η(ζ) = ζ(0, 1) and θ(ξ) = ζ(0, 1).

If ζ is type II and periodic of exact period n, we say ζ is

◮ indifferent (or neutral) if degζ φn = 1.

◮ repelling if degζ φn ≥ 2.

Warning: Repelling type II points (usually) do not actually repelin most directions.

Note: Periodic type III and IV points are always indifferent.

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Berkovich Fatou and Julia Sets

DefinitionAn open set U ⊆ P1

Ber is dynamically stable under φ ∈ CK (z) if⋃

n≥0

φn(U) omits infinitely many points of P1Ber.

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Berkovich Fatou and Julia Sets

DefinitionAn open set U ⊆ P1

Ber is dynamically stable under φ ∈ CK (z) if⋃

n≥0

φn(U) omits infinitely many points of P1Ber.

The (Berkovich) Fatou set of φ is the set FBer = Fφ,Ber given by

FBer := {x ∈ P1Ber : x has a dynamically stable neighborhood}.

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Berkovich Fatou and Julia Sets

DefinitionAn open set U ⊆ P1

Ber is dynamically stable under φ ∈ CK (z) if⋃

n≥0

φn(U) omits infinitely many points of P1Ber.

The (Berkovich) Fatou set of φ is the set FBer = Fφ,Ber given by

FBer := {x ∈ P1Ber : x has a dynamically stable neighborhood}.

The (Berkovich) Julia set of φ is the set

JBer = Jφ,Ber := P1Ber r Fφ,Ber.

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Basic Properties of Berkovich Fatou and Julia Sets

◮ FBer is open, and JBer is closed.

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Basic Properties of Berkovich Fatou and Julia Sets

◮ FBer is open, and JBer is closed.

◮ Fφn,Ber = Fφ,Ber, and Jφn,Ber = Jφ,Ber

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Basic Properties of Berkovich Fatou and Julia Sets

◮ FBer is open, and JBer is closed.

◮ Fφn,Ber = Fφ,Ber, and Jφn,Ber = Jφ,Ber

◮ φ(FBer) = FBer = φ−1(FBer), andφ(JBer) = JBer = φ−1(JBer).

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Basic Properties of Berkovich Fatou and Julia Sets

◮ FBer is open, and JBer is closed.

◮ Fφn,Ber = Fφ,Ber, and Jφn,Ber = Jφ,Ber

◮ φ(FBer) = FBer = φ−1(FBer), andφ(JBer) = JBer = φ−1(JBer).

◮ F = FBer ∩ P1(CK ), and J = JBer ∩ P

1(CK ).

Page 76: Non-archimedean Dynamics in Dimension One: Lecture 2swc.math.arizona.edu/aws/2010/2010BenedettoLectureNotes2.pdf · There are ways to get around that (see Section 5 of the lecture

Basic Properties of Berkovich Fatou and Julia Sets

◮ FBer is open, and JBer is closed.

◮ Fφn,Ber = Fφ,Ber, and Jφn,Ber = Jφ,Ber

◮ φ(FBer) = FBer = φ−1(FBer), andφ(JBer) = JBer = φ−1(JBer).

◮ F = FBer ∩ P1(CK ), and J = JBer ∩ P

1(CK ).

◮ All attracting periodic points are Fatou.

◮ All repelling periodic points are Julia.

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Basic Properties of Berkovich Fatou and Julia Sets

◮ FBer is open, and JBer is closed.

◮ Fφn,Ber = Fφ,Ber, and Jφn,Ber = Jφ,Ber

◮ φ(FBer) = FBer = φ−1(FBer), andφ(JBer) = JBer = φ−1(JBer).

◮ F = FBer ∩ P1(CK ), and J = JBer ∩ P

1(CK ).

◮ All attracting periodic points are Fatou.

◮ All repelling periodic points are Julia.

◮ Indifferent periodic type II points are Fatou if the residue fieldis algebraic over a finite field,

Page 78: Non-archimedean Dynamics in Dimension One: Lecture 2swc.math.arizona.edu/aws/2010/2010BenedettoLectureNotes2.pdf · There are ways to get around that (see Section 5 of the lecture

Basic Properties of Berkovich Fatou and Julia Sets

◮ FBer is open, and JBer is closed.

◮ Fφn,Ber = Fφ,Ber, and Jφn,Ber = Jφ,Ber

◮ φ(FBer) = FBer = φ−1(FBer), andφ(JBer) = JBer = φ−1(JBer).

◮ F = FBer ∩ P1(CK ), and J = JBer ∩ P

1(CK ).

◮ All attracting periodic points are Fatou.

◮ All repelling periodic points are Julia.

◮ Indifferent periodic type II points are Fatou if the residue fieldis algebraic over a finite field, but they can be Julia otherwise.

In general, if ζ(0, 1) is fixed by φ,and if φ

m(z) = z for some m ≥ 1,

then ζ(0, 1) is Fatou.

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P1(C), P

1(CK ), and P1Ber

P1(C) P

1(CK ) P1Ber

Some indifferent All indifferent Most indifferentpoints are Fatou, points are Fatou points are Fatou.and some are Julia

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P1(C), P

1(CK ), and P1Ber

P1(C) P

1(CK ) P1Ber

Some indifferent All indifferent Most indifferentpoints are Fatou, points are Fatou points are Fatou.and some are Julia

J is compact J may not JBer is compactbe compact

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P1(C), P

1(CK ), and P1Ber

P1(C) P

1(CK ) P1Ber

Some indifferent All indifferent Most indifferentpoints are Fatou, points are Fatou points are Fatou.and some are Julia

J is compact J may not JBer is compactbe compact

J is nonempty J may be empty JBer is nonempty

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P1(C), P

1(CK ), and P1Ber

P1(C) P

1(CK ) P1Ber

Some indifferent All indifferent Most indifferentpoints are Fatou, points are Fatou points are Fatou.and some are Julia

J is compact J may not JBer is compactbe compact

J is nonempty J may be empty JBer is nonempty

F may be empty F is nonempty FBer is nonempty

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P1(C), P

1(CK ), and P1Ber

P1(C) P

1(CK ) P1Ber

Some indifferent All indifferent Most indifferentpoints are Fatou, points are Fatou points are Fatou.and some are Julia

J is compact J may not JBer is compactbe compact

J is nonempty J may be empty JBer is nonempty

F may be empty F is nonempty FBer is nonempty

J is the closure JBer is the closureof the set of ??? of the set ofrepelling periodic (see Project #1) repelling periodicpoints (Type I & II) points