Variation of canonical height, illustrated Laura DeMarco - - PowerPoint PPT Presentation

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Variation of canonical height, illustrated Laura DeMarco - - PowerPoint PPT Presentation

Variation of canonical height, illustrated Laura DeMarco Northwestern University Theorem I.0.3. (Silverman, VCH I, 1992) P = (0 , 0) E = { y 2 + Txy + Ty = x 3 + 2 Tx 3 } (log 2) 2 h E t ( P t ) = 1 15 log t + 2 25 log 2 + 2 log( t 5 / 2) +


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Variation of canonical height, illustrated

Laura DeMarco Northwestern University

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E = {y2 + Txy + Ty = x3 + 2Tx3} Theorem I.0.3. (Silverman, VCH I, 1992) P = (0, 0) ˆ hEt(Pt) = 1 15 log t + 2 25 log 2 + 2 25 (log 2)2 log(t5/2) + O(t−1) for t ∈ Z, t → ∞

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  • Brief overview:

families of elliptic curves

  • Connections with dynamics
  • pictures
  • Rationality of canonical heights?

(work in progress with Dragos Ghioca)

Variation of canonical height, illustrated

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E = elliptic curve / number field K

y2 = x3 + Ax + B

A, B ∈ K

ˆ hE(P) = lim

n→∞

1 4n hWeil([2nP]x)

N´ eron-Tate (canonical) height function

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E = elliptic curve / number field K

y2 = x3 + Ax + B

A, B ∈ K

ˆ hE(P) = lim

n→∞

1 4n hWeil([2nP]x)

N´ eron-Tate (canonical) height function X P t Et

k = K(X) E = elliptic curve / function field k P ∈ E(k) Study ˆ hEt(Pt) for t ∈ X( ¯ K)

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E = elliptic curve / number field K

y2 = x3 + Ax + B

A, B ∈ K

ˆ hE(P) = lim

n→∞

1 4n hWeil([2nP]x)

N´ eron-Tate (canonical) height function X P t Et

k = K(X) E = elliptic curve / function field k P ∈ E(k) Study ˆ hEt(Pt) for t ∈ X( ¯ K)

  • Theorem. (Silverman, 1983)
  • Theorem. (Tate, 1983)

ˆ hEt(Pt) = hX,DP (t) + O(1) lim

hX(t)→∞

ˆ hEt(Pt) hX(t) = ˆ hE(P)

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E = elliptic curve / number field K

y2 = x3 + Ax + B

A, B ∈ K

ˆ hE(P) = lim

n→∞

1 4n hWeil([2nP]x)

N´ eron-Tate (canonical) height function X P t Et

k = K(X) E = elliptic curve / function field k P ∈ E(k) Study ˆ hEt(Pt) for t ∈ X( ¯ K)

  • Theorem. (Silverman, 1983)
  • Theorem. (Tate, 1983)

ˆ hEt(Pt) = hX,DP (t) + O(1) lim

hX(t)→∞

ˆ hEt(Pt) hX(t) = ˆ hE(P)

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Silverman’s VCH I, II, III, 1992-1994

ˆ hEt(Pt) = X

v∈MK

ˆ λEt,v(Pt)

satisfy The components in the local decomposition

(1) ˆ λEt,v(Pt) = ˆ λE,t0(P) log |u(t)|v + continuous correction term (2) correction term ≡ 0 for all but finitely many v ∈ MK

for t near t0 ∈ X( ¯ K).

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Silverman’s VCH I, II, III, 1992-1994

“I’ve always thought it was intriguing that the difference h(P_t) - h(P)h(t) is [so well behaved]. On the other hand, I’ve never found a good application.”

  • Joe Silverman, July 20, 2015

ˆ hEt(Pt) = X

v∈MK

ˆ λEt,v(Pt)

satisfy The components in the local decomposition

(1) ˆ λEt,v(Pt) = ˆ λE,t0(P) log |u(t)|v + continuous correction term (2) correction term ≡ 0 for all but finitely many v ∈ MK

for t near t0 ∈ X( ¯ K).

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= ⇒ we are set up to study the distribution of “small” points on X = ⇒ ˆ hEt(Pt) defines a “good height function” on X( ¯ K)

(e.g. Baker--Rumely, Chambert-Loir, Favre--Rivera-Letelier 2006, Yuan 2008)

ˆ hEt(Pt) = X

v∈MK

ˆ λEt,v(Pt)

satisfy The components in the local decomposition

(1) ˆ λEt,v(Pt) = ˆ λE,t0(P) log |u(t)|v + continuous correction term (2) correction term ≡ 0 for all but finitely many v ∈ MK

for t near t0 ∈ X( ¯ K).

Silverman’s VCH I, II, III, 1992-1994

i.e., a continuous potential function for an adelic measure µ = {µv} (or an adelic metrized line bundle, in sense of Zhang, 1995)

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ˆ hEt(Pt) = X

v∈MK

ˆ λEt,v(Pt)

What are these measures on X?

(strictly speaking, the measures live on the Berkovich analytification of X)

P ∈ E(k) K = number field E = elliptic curve / function field k = K(X) (1) ˆ λEt,v(Pt) = ˆ λE,t0(P) log |u(t)|v + continuous correction term (2) correction term ≡ 0 for all but finitely many v ∈ MK µv = ∆(correction term)

X

P t

Et

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ˆ hEt(Pt) = X

v∈MK

ˆ λEt,v(Pt)

What are these measures on X?

(strictly speaking, the measures live on the Berkovich analytification of X)

P ∈ E(k) K = number field E = elliptic curve / function field k = K(X) (1) ˆ λEt,v(Pt) = ˆ λE,t0(P) log |u(t)|v + continuous correction term (2) correction term ≡ 0 for all but finitely many v ∈ MK µv = ∆(correction term)

The measure is a pull-back of the Haar measures on the elliptic curves. This is a special case of the dynamical bifurcation measure and the correction term governs the “intensity” of the bifurcation.

X

P t

Et

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Call-Silverman canonical height (1994)

f : P1 → P1 ˆ hf : P1( ¯ K) → R ˆ hf(f(z)) = (deg f)ˆ hf(z) ˆ hf(z) = h(z) + O(1) determined uniquely by two properties: ˆ hf(z) = lim

n→∞

1 (deg f)n h(f n(z)) = X

v∈MK

ˆ λf,v(z)

The variation of the canonical height -- at the archimedean place -- quantifies bifurcations in a traditional dynamical sense.

{

Study variation ˆ hft(Pt) for t ∈ X, in families {ft}. Take the Laplacian ∆ of the local heights, as functions of t.

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Example: degree 2 polynomials

ft(z) = z2 + t t ∈ C P = 0

The Mandelbrot set

ˆ λft,v=∞(Pt) = 1 2 log |t| + correction term

Bifurcation measure µP is harmonic measure on ∂M

(Douady-Hubbard, Sibony 1981, Ma˜ n´ e-Sad-Sullivan 1983)

for |t| large

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Example: degree 2 polynomials

ft(z) = z2 + t t ∈ C P = 1

A Mandelbrot-like set

(Baker-D. 2011)

ˆ λft,v=∞(Pt) = 1 2 log |t| + correction term

Bifurcation measure µP is harmonic measure on ∂M

Used to answer an “unlikely intersections” question posed by Zannier: there are only finitely many t for which both 0 and 1 have finite orbit for ft.

for |t| large

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In these examples, the measures are compactly supported (away from point of bad reduction at infinity). So the “correction terms” will be nice harmonic functions near infinity. For general families of polynomials, height functions and measures depend

  • nly on rates of escape to infinity. Ingram proved the analog of Tate’s 1983 result:
  • Theorem. (Ingram, 2012)

ˆ hft(Pt) = hX,DP (t) + O(1)

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Example, in the context of Silverman’s VCH I,II, III

Et = {y2 = x(x − 1)(x − t)}

P = (a, p a(a − 1)(a − t)) (1) ˆ λEt,v(Pt) = ˆ λE,t0(P) log |u(t)|v + continuous correction term µv = ∆(correction term)

(D.-Wang-Ye, 2015) building on the results

  • f (Masser-Zannier, 2008, 2010, 2012)

a ∈ Q(t) Fact 1. The parameters t ∈ X where Pt is torsion on Et are equidistributed with respect to these measures µP,v. Fact 2. The measures {µPv} coincide with {µQv} if and only if the points P and Q are linearly related on E. This can be seen already at the archimedean place. (2) correction term ≡ 0 for all but finitely many v ∈ MK

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a = 2 −3 < Re t < 5 −4 < Im t < 4

5

Plot: parameters t where a is the x-coordinate

  • f a torsion

point on Et,

  • f order 2n

with n < 8.

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a = 2 −3 < Re t < 5 −4 < Im t < 4 Plot: parameters t where a is the x-coordinate

  • f a torsion

point on Et,

  • f order 2n

with n < 10.

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a = 2 −3 < Re t < 5 −4 < Im t < 4 Plot: parameters t where a is the x-coordinate

  • f a torsion

point on Et,

  • f order 2n

with n < 15.

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−3 < Re t < 5 −4 < Im t < 4 Plot: parameters t where a is the x-coordinate

  • f a torsion

point on Et,

  • f order 2n

with n < 15. a = 5 a = 5

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µa = µb if and only if a = b a = 2 b = 5 Et = {y2 = x(x − 1)(x − t)} The Haar measure on Et pushed down to P1 is µt = C(t) |z(z − 1)(z − t)| |dz|2 where C(t) = 2|t(t − 1)|ρΣ(t).

Density for hyperbolic metric on triply-punctured sphere (McMullen)

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µa = µb if and only if a = b a = 2 b = 5 Et = {y2 = x(x − 1)(x − t)}

gt(z) = 2C(t) Z

P1

log |z − ζ| |ζ(ζ − 1)(ζ − t)| |dζ|2

Potential function for µt: = ⇒ Potential function for µa:

ga(t) = 2C(t) Z

P1

log |a − ζ| |ζ(ζ − 1)(ζ − t)| |dζ|2

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ˆ hEt(Pt) = X

v∈MK

ˆ λEt,v(Pt)

satisfy The components in the local decomposition

(1) ˆ λEt,v(Pt) = ˆ λE,t0(P) log |u(t)|v + continuous correction term (2) correction term ≡ 0 for all but finitely many v ∈ MK

for t near t0 ∈ X( ¯ K).

P ∈ E(k) K = number field E = elliptic curve / function field k = K(X)

  • Theorem. (Silverman)

Known for: Latt`es maps (a corollary of above) Particular families of polynomials and rational maps (Baker-D., D.-Wang-Ye, Ghioca-Hsia-Tucker, Ghioca-Mavraki, Ingram)

What do we know for dynamical canonical height?

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ˆ hEt(Pt) = X

v∈MK

ˆ λEt,v(Pt)

satisfy The components in the local decomposition

(1) ˆ λEt,v(Pt) = ˆ λE,t0(P) log |u(t)|v + continuous correction term (2) correction term ≡ 0 for all but finitely many v ∈ MK

for t near t0 ∈ X( ¯ K).

P ∈ E(k) K = number field E = elliptic curve / function field k = K(X)

  • Theorem. (Silverman)

Known for: Latt`es maps (a corollary of above) Particular families of polynomials and rational maps (Baker-D., D.-Wang-Ye, Ghioca-Hsia-Tucker, Ghioca-Mavraki, Ingram)

Don’t know in general, but expect to be true

What do we know for dynamical canonical height?

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ˆ hEt(Pt) = X

v∈MK

ˆ λEt,v(Pt)

satisfy The components in the local decomposition

(1) ˆ λEt,v(Pt) = ˆ λE,t0(P) log |u(t)|v + continuous correction term (2) correction term ≡ 0 for all but finitely many v ∈ MK

for t near t0 ∈ X( ¯ K).

P ∈ E(k) K = number field E = elliptic curve / function field k = K(X)

  • Theorem. (Silverman)

Known for: Latt`es maps (a corollary of above) Particular families of polynomials and rational maps (Baker-D., D.-Wang-Ye, Ghioca-Hsia-Tucker, Ghioca-Mavraki, Ingram)

Don’t know in general, but expect to be true False for general dynamical families! (D.-Wang-Ye, 2015)

What do we know for dynamical canonical height?

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ˆ hEt(Pt) = X

v∈MK

ˆ λEt,v(Pt)

satisfy The components in the local decomposition

(1) ˆ λEt,v(Pt) = ˆ λE,t0(P) log |u(t)|v + continuous correction term

for t near t0 ∈ X( ¯ K).

P ∈ E(k) K = number field E = elliptic curve / function field k = K(X)

  • Theorem. (Silverman)

A more basic question: do we understand the leading terms?

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ˆ hEt(Pt) = X

v∈MK

ˆ λEt,v(Pt)

satisfy The components in the local decomposition

(1) ˆ λEt,v(Pt) = ˆ λE,t0(P) log |u(t)|v + continuous correction term

for t near t0 ∈ X( ¯ K).

P ∈ E(k) K = number field E = elliptic curve / function field k = K(X)

  • Theorem. (Silverman)

A more basic question: do we understand the leading terms?

  • Fact. ˆ

hE(P) and ˆ λE,t0(P) are rational numbers.

  • Explanation. These are intersection numbers on a N´

eron model. Another Fact. The analogous “weak” N´ eron models do not always exist in the dynamical setting. (Call-Silverman, Hsia)

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Rationality of canonical height

(work in progress with Dragos Ghioca)

  • 1. There is a dynamical proof that local/global canonical heights

are always rational for elliptic curves.

0.0 0.2 0.4 0.6 0.8 1.0 0.2 0.4 0.6 0.8 1.0

Idea: Dynamics of the multiplication-by-2 map on the Berkovich P1, Julia set is an interval. Action is by the tent map of slope 2, all rational points are preperiodic. (Favre, Rivera-Letelier)

  • Theorem. (Ingram, 2012)

For polynomials, local heights at non-archimedean places are rational.

Compare: The tent map of slope 2

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J1 J−1 J0

ζ−9 ζ9 ζ−1,9 ζ1,9 ζ−6 ζ−3 ζ0 3 3 6 1

{

I1 I2{

{

I3 ∞ 1 −1

  • 2. There exist rational functions and points with irrational local

heights!

Rationality of canonical height

(work in progress with Dragos Ghioca)

Idea: Julia set contains forward invariant intervals in the Berkovich space AND classical points. There are Cantor sets of points containing aperiodic itineraries.

ft(z) = t18z6 + 1 t18z6 + z(z − 1)(z + 1)

(Bajpai, Benedetto, Chen, Kim, Marschall, Onul, Xiao)

k = ¯ Q((t))

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J1 J−1 J0

ζ−9 ζ9 ζ−1,9 ζ1,9 ζ−6 ζ−3 ζ0 3 3 6 1

{

I1 I2{

{

I3 ∞ 1 −1

  • 2. There exist rational functions and points with irrational local

heights!

Rationality of canonical height

(work in progress with Dragos Ghioca)

Idea: Julia set contains forward invariant intervals in the Berkovich space AND classical points. There are Cantor sets of points containing aperiodic itineraries.

ft(z) = t18z6 + 1 t18z6 + z(z − 1)(z + 1)

(Bajpai, Benedetto, Chen, Kim, Marschall, Onul, Xiao)

BUT, we expect these points to be transcendental...

(Fatou, Bell-Bruin-Coons, Adamczewski-Bell)

k = ¯ Q((t))

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Next steps

  • Question. Is the canonical height ˆ

hf(P) rational?

  • Question. Is there a good intersection-theoretic description of ˆ

hf(P), even in the absence of (weak) N´ eron models?

  • Question. Are the pieces in the local decomposition of ˆ

hft(Pt) “nice” functions of t?

  • Question. Is there a divisor DP ∈ Pic(X) ⊗ Q so that

k = K(X), f : P1 → P1 defined over k, P ∈ P1(¯ k) ˆ hft(Pt) = hX,DP (t) + O(1)

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Thank you, Joe, for providing so many great ideas and inspiration!

E = {y2 + Txy + Ty = x3 + 2Tx3} Theorem I.0.3. (Silverman, VCH I, 1992) P = (0, 0) ˆ hEt(Pt) = 1 15 log t + 2 25 log 2 + 2 25 (log 2)2 log(t5/2) + O(t−1) for t ∈ Z, t → ∞