heights and dynamics over arbitrary fields
TRANSCRIPT
Rigidity of Dynamical systems
Theorem (Yuan-Zhang, C.)
Let f , g : X → X be two polarizable algebraic dynamical systems definedover any field. The following are equivalent:
1 Prep(f ) ⊂ Prep(g).
2 Prep(f ) ∩ Prep(g) is Zariski dense in X .
3 Prep(f ) = Prep(g).
Remarks
Proven by Yuan-Zhang in characteristic zero, by C. for positivecharacteristic.
Prep(f ) is always dense in X (Fakhruddin).
Alex Carney, University of Rochester Heights and dynamics over arbitrary fields 1/21
Proof Outline
1 Define heights over finitely generated fields.
2 Construct canonical heights hf and hg , and equate canonical heightzero points and preperiodic points via Northcott.
3 Relate hf and hg using arithmetic intersection theory (Hodge IndexTheorem) over finitely generated fields.
Alex Carney, University of Rochester Heights and dynamics over arbitrary fields 2/21
1. Base k and base Z
Let K be a finitely generated extension of a field k .
We consider two cases
1 Base Zk = Qd = tr.deg(K/k)All models are schemes over SpecZ.
2 Base k
k can be any field (incl. Q)d + 1 = tr.deg(K/k)All models are schemes over Spec k.
Example
K/k = Q(t)/Q can be base Z (d=1) or base k (d=0).
Alex Carney, University of Rochester Heights and dynamics over arbitrary fields 3/21
Existing Theory, R-valued heights
Base Z: Moriwaki heights
Base k: Geometric heights (Lang, Serre, others)
But these require a polarization:
1 A model B for K , over Spec k or SpecZ.
2 (Hermitian, in base Z) line bundles H1, . . . ,Hd on B.
This determines a set of absolute values satisfying the product formulavia intersections on B.
Problem
Polarizations are only unique when d = 0.
Alex Carney, University of Rochester Heights and dynamics over arbitrary fields 4/21
Models over k and Z
Fix a projective K -variety X .
Open Models
An open arithmetic model for X is a quasi-projective integral schemeover the base (k or Z), whose base change to K is X .
· · · ↪−→W2 ↪−→W1
They form an inverse system via inclusion.
Projective models
A projective model X for an open model W is an open embeddingW ↪→ X into a projective arithmetic model, such that X\W is thesupport of an effective Cartier divisor.
· · · −→ X2 −→ X1
They form an inverse system via dominant morphisms.
Alex Carney, University of Rochester Heights and dynamics over arbitrary fields 5/21
Limits of models
Limits of projective models
For an open model U for X , define
Pic(U) := lim−→X
Pic(X )Q
over the inverse system of projective models for UPic(U)cont = completion w/r/t partial ordering by effectivity on X\U .
Limits of open models
Pic(X ) := lim−−−→U→V
Pic(U)cont
over the inverse system of flat maps U → V of open arithmetic modelsfor X → SpecK .
Special case: Pic(K ) := Pic(SpecK ).
Alex Carney, University of Rochester Heights and dynamics over arbitrary fields 6/21
A relative intersection pairing
Let X → Y be a morphism of projective K -varieties of pure dimension n.
The vector-valued product
Pic(X )n+1 −→ Pic(Y )
(L0, . . . , Ln) 7→ L0 · · · Ln
Defined via the Deligne pairing.
Important case: Y = SpecK .
The R-valued product
Pic(K )d+1 −→ R
(H0, . . . ,Hd) 7→ H0 · · ·Hd
Pic(K )-valued product + polarization = R-valued product.
Alex Carney, University of Rochester Heights and dynamics over arbitrary fields 7/21
Vector valued heights
The Pic(K ) height
Fix L ∈ Pic(X ) and Z a closed subvariety of X . Define
hL(Z ) :=
(L|Z)dim Z+1
(d + 1) (L|Z )dim Z∈ Pic(K )
When x is a K -point, hL(x) = π∗(L|x)/[K (x) : K ].
Relation to existing heights
d = 0: hL is a Q-line bundle on the unique model for K , its degreeis the usual (geometric) height.
d > 0: Fix a polarization H1, . . . ,Hd . The R-producthL(Z ) · H1 · · ·Hd is the Moriwaki/geometric height.
Alex Carney, University of Rochester Heights and dynamics over arbitrary fields 8/21
Proof Outline
1 Define heights over finitely generated fields.
2 Construct canonical heights hf and hg , and equate canonical heightzero points and preperiodic points via Northcott.
3 Relate hf and hg using arithmetic intersection theory (Hodge IndexTheorem) over finitely generated fields.
Alex Carney, University of Rochester Heights and dynamics over arbitrary fields 9/21
Canonical heights
Let f : X → X be a dynamical system with a polarizationf ∗L = qL = L⊗q for L ample, q > 1.
Definition
A canonical height hf for f is a height such that
hf (f (x)) = qhf (x).
Tate’s limiting argument
1 Extend L to some L ∈ Pic(X ).
2 Set Lf := limn→∞
1
qn(f n)∗L, show this converges.
3 hf := hLf.
Alex Carney, University of Rochester Heights and dynamics over arbitrary fields 10/21
Isotriviality and base k
Suppose we are in the base k setting.
Theorem (Baker)
Suppose f : P1K → P1
K is a rational function. The set{x ∈ P1(K ) : hf (x) = 0} is finite ⇔ k = Fq or f is not isotrivial.
Definition
Let A be an abelian K -variety. Chow’s K/k-trace is an abelian k-varietyTrK/k(A) with a map τ : TrK/k(A)K → A, universal for all maps from anabelian k-variety to A.
Theorem (Lang-Neron)
Let hNT = h[2] be the Neron-Tate height on A. Then hNT(x) = 0 ⇔ x istorsion or x ∈ TrK/k(A)(k).
Alex Carney, University of Rochester Heights and dynamics over arbitrary fields 11/21
Constructible isotriviality
Definition
A constructible map is a composition of rational maps and inversesof totally inseparable rational maps.
A dynamical system f : X → X is constructibly isotrivial providedthere exists a rational map g : Y → Y defined over k such that(X , f ) is constructibly isomorphic to (YK , gK ).
(X , f ) is totally non-isotrivial provided neither (X , f ) itself nor anypositive dimensional periodic closed subvariety of (X , f ) isconstructibly isotrivial.
Example
E = supersingular elliptic curve over k , and Γ = order p subgroupscheme of E [p]× E [p]. Then (EK × EK )/Γ is constructibly isotrivial, butnot isotrivial. τ has a finite kernel.
Alex Carney, University of Rochester Heights and dynamics over arbitrary fields 12/21
The Northcott Principle
Definition
For M ∈ Pic(K ), write M ≡ 0 to mean M is numerically trivial.
Theorem (Northcott, base Z, Yuan-Zhang 2013)
Let X be projective over K , L ∈ Pic(X ) ample, and α ∈ Pic(K ). The set
{x ∈ X (K ) : hL(x) ≤ α}
is finite.
Theorem (Northcott, base k , Gauthier-Vigny 2019, C. 2020)
Let f : X → X be polarizable, and suppose k is finite or (X , f ) is totallynon-isotrivial. Then
{x ∈ X (K ) : hf (x) ≡ 0}
is finite.
Alex Carney, University of Rochester Heights and dynamics over arbitrary fields 13/21
Proof
Base Z
1 Fix a polarization ⇒ Moriwaki height.
2 Northcott proven by Moriwaki for this R-height.
3 Height approximated uniformly as the polarization varies.
Base k
1 Fix a polarization ⇒ Geometric height.
2 k = Fq: Known for geometric heights.
3 Chatzidakis-Hrushovski (Model theory):limited set dense ⇒ constructibly isotrivial.
4 Induct on dimension.
5 Vary the polarization.
Alex Carney, University of Rochester Heights and dynamics over arbitrary fields 14/21
Relative heights in function fields
Let K/k1/k be a tower of finitely generated extensions, and f : X → X apolarizable dynamical system over K .
Two relative heights on K
Height relative to K/k Height relative to K/k1
Values in Pic(K ) = Pic(K/k) Values in Pic(K ) = Pic(K/k1)
Northcott ⇔ non-isotriviality /k Northcott ⇔ non-isotriviality /k1
K/k height intersected with pullbacks from Pic(k1/k) ⇒ K/k1 height.
Example
Let K = C(t).
If (X , f ) totally non-isotrivial over C, use C(t)/C height.
If not, find f.g. subfield of definition K , use K/Q height.
Alex Carney, University of Rochester Heights and dynamics over arbitrary fields 15/21
Outline
1 Define heights over finitely generated fields.
2 Construct canonical heights hf and hg , and equate canonical heightzero points and preperiodic points via Northcott.
3 Relate hf and hg using arithmetic intersection theory (Hodge IndexTheorem) over finitely generated fields.
Alex Carney, University of Rochester Heights and dynamics over arbitrary fields 16/21
The Hodge Index Theorem
Theorem (Yuan-Zhang 2013, C. 2020)
Let π : X → SpecK be a projective variety of dimension n. Let
M, L2, . . . , Ln ∈ Pic(X ) with L2, . . . , Ln ample and M · L2 · · · Ln = 0.Then
1 (Inequality)
M2 · L2 · · · Ln ≤ 0.
2 (Equality) Further,
M2 · L2 · · · Ln ≡ 0
if and only if
M ∈ π∗Pic(K )int + TrK/k Pic0(X ).
Alex Carney, University of Rochester Heights and dynamics over arbitrary fields 17/21
Proof Sketch
Case d = 0 (I.e. number fields/transcendence degree 1 function fields)proven by Yuan-Zhang/C.
Lemma
Let X be a curve, and M ∈ Pic0(X ). Then M has a unique extension to
M0 ∈ Pic(X ) with M0 = M, for which
M2
0 = −2hNT(M),
where hNT is the vector-valued Neron-Tate canonical height on JacX .
Follows Faltings’ Calculus on arithmetic surfaces/Hriljac’s thesis.
Address M −M0 by studying intersections of fibers.
Induct on the dimension of X .
Alex Carney, University of Rochester Heights and dynamics over arbitrary fields 18/21
Proving rigidity of dynamical systems
Preperiodic points always have height zero (doesn’t require Northcott).
The Lefschetz Principle
X , f , g and their polarizations are all defined over some field K which isfinitely generated over either Q or Fq.
Northcott always holds.
Thus canonical height zero points are all preperiodic (entire forwardorbit has height zero).
Proof sketch
1 Construct canonical heights hLfand hMg
.
2 Show Prep(f ) ∩ Prep(g) dense in X ⇒ hLf +Mg(X ) ≡ 0.
3 Apply Hodge Index Theorem to Lf −Mg .
Alex Carney, University of Rochester Heights and dynamics over arbitrary fields 19/21
Future directions
Applications to Unlikely Intersections, higher dimensional families.
Better understand constructible isotriviality
Develop vector space structure of Pic(K ) further.
Alex Carney, University of Rochester Heights and dynamics over arbitrary fields 20/21