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(1)

Second descent and rational points on Kummer surfaces

Yonatan Harpaz

IH´ES

Luminy, September 2016

(2)

Rational points

Let X be a smooth projective variety defined over a number field.

Question

Suppose that X has points everywhere locally.

Does it have a rational point?

Probably not in general.

Conditional counter-examples constructed by Sarnak & Wang, Poonen and Smeets.

No unconditional counter-example is known.

(3)

Rational points

Let X be a smooth projective variety defined over a number field.

Question

Suppose that X has points everywhere locally.

Does it have a rational point?

Probably not in general.

Conditional counter-examples constructed by Sarnak & Wang, Poonen and Smeets.

No unconditional counter-example is known.

(4)

Rational points

Let X be a smooth projective variety defined over a number field.

Question

Suppose that X has points everywhere locally. Does it have a rational point?

Probably not in general.

Conditional counter-examples constructed by Sarnak & Wang, Poonen and Smeets.

No unconditional counter-example is known.

(5)

Rational points

Let X be a smooth projective variety defined over a number field.

Question

Suppose that X has points everywhere locally and no Brauer-Manin obstruction. Does it have a rational point?

Probably not in general.

Conditional counter-examples constructed by Sarnak & Wang, Poonen and Smeets.

No unconditional counter-example is known.

(6)

Rational points

Let X be a smooth projective variety defined over a number field.

Question

Suppose that X is simply-connected, has points everywhere locally and no Brauer-Manin obstruction. Does it have a rational point?

Probably not in general.

Conditional counter-examples constructed by Sarnak & Wang, Poonen and Smeets.

No unconditional counter-example is known.

(7)

Rational points

Let X be a smooth projective variety defined over a number field.

Question

Suppose that X is simply-connected, has points everywhere locally and no Brauer-Manin obstruction. Does it have a rational point?

Probably not in general.

Conditional counter-examples constructed by Sarnak & Wang, Poonen and Smeets.

No unconditional counter-example is known.

(8)

Rational points

Let X be a smooth projective variety defined over a number field.

Question

Suppose that X is simply-connected, has points everywhere locally and no Brauer-Manin obstruction. Does it have a rational point?

Probably not in general.

Conditional counter-examples constructed by Sarnak & Wang, Poonen and Smeets.

No unconditional counter-example is known.

(9)

Rational points

Let X be a smooth projective variety defined over a number field.

Question

Suppose that X is simply-connected, has points everywhere locally and no Brauer-Manin obstruction. Does it have a rational point?

Probably not in general.

Conditional counter-examples constructed by Sarnak & Wang, Poonen and Smeets.

No unconditional counter-example is known.

(10)

Rational points on surfaces

Let X be a smooth projective surface defined over a number field.

Question

Suppose that X is simply-connected, has points everywhere locally and no Brauer-Manin obstruction. Does it have a rational point?

Probably yes when X is a rational surface (conjectured by Colliot-th´ el` ene and Sansuc in the 1979).

Probably not always when X is of general type. What about K3 surfaces?

Conjecture (Skorobogatov)

The Brauer-Manin obstruction is the only obstruction for the

Hasse principle on smooth and proper K3 surfaces.

(11)

Rational points on surfaces

Let X be a smooth projective surface defined over a number field.

Question

Suppose that X is simply-connected, has points everywhere locally and no Brauer-Manin obstruction. Does it have a rational point?

Probably yes when X is a rational surface (conjectured by Colliot-th´ el` ene and Sansuc in the 1979).

Probably not always when X is of general type. What about K3 surfaces?

Conjecture (Skorobogatov)

The Brauer-Manin obstruction is the only obstruction for the

Hasse principle on smooth and proper K3 surfaces.

(12)

Rational points on surfaces

Let X be a smooth projective surface defined over a number field.

Question

Suppose that X is simply-connected, has points everywhere locally and no Brauer-Manin obstruction. Does it have a rational point?

Probably yes when X is a rational surface (conjectured by Colliot-th´ el` ene and Sansuc in the 1979).

Probably not always when X is of general type.

What about K3 surfaces? Conjecture (Skorobogatov)

The Brauer-Manin obstruction is the only obstruction for the

Hasse principle on smooth and proper K3 surfaces.

(13)

Rational points on surfaces

Let X be a smooth projective surface defined over a number field.

Question

Suppose that X is simply-connected, has points everywhere locally and no Brauer-Manin obstruction. Does it have a rational point?

Probably yes when X is a rational surface (conjectured by Colliot-th´ el` ene and Sansuc in the 1979).

Probably not always when X is of general type.

What about K3 surfaces?

Conjecture (Skorobogatov)

The Brauer-Manin obstruction is the only obstruction for the

Hasse principle on smooth and proper K3 surfaces.

(14)

Rational points on surfaces

Let X be a smooth projective surface defined over a number field.

Question

Suppose that X is simply-connected, has points everywhere locally and no Brauer-Manin obstruction. Does it have a rational point?

Probably yes when X is a rational surface (conjectured by Colliot-th´ el` ene and Sansuc in the 1979).

Probably not always when X is of general type.

What about K3 surfaces?

Conjecture (Skorobogatov)

The Brauer-Manin obstruction is the only obstruction for the

(15)

Kummer Surfaces

Special case - Kummer surfaces.

k - a number field;

A - an abelian surface over k ;

Y

α

−→ A - a 2-covering, by which we mean a twist of the map A −→

2

A by a class α ∈ H

1

(k, A[2]).

ι : A → A, ι(x) = −x, also acts compatibly on Y

α

;

X

α

= Kum(Y

α

) := the minimal desingularisation of Y

α

/ι, is called the Kummer surface attached to Y

α

.

F /k quadratic ⇒ A

F

[2] ∼ = A[2] and α interpreted in H

1

(k, A

F

[2]) classifies the 2-covering Y

αF

−→ A

F

.

X

α

∼ = Kum(Y

αF

) for every quadratic extension F /k. {A

F

}

F/k

- the abelian surfaces associated to X

α

. Diophantine problem of interest

Assuming finiteness of X for all associated abelian surfaces, find

sufficient conditions for the Hasse principle to hold on X

α

.

(16)

Kummer Surfaces

Special case - Kummer surfaces.

k - a number field;

A - an abelian surface over k ;

Y

α

−→ A - a 2-covering, by which we mean a twist of the map A −→

2

A by a class α ∈ H

1

(k, A[2]).

ι : A → A, ι(x) = −x, also acts compatibly on Y

α

;

X

α

= Kum(Y

α

) := the minimal desingularisation of Y

α

/ι, is called the Kummer surface attached to Y

α

.

F /k quadratic ⇒ A

F

[2] ∼ = A[2] and α interpreted in H

1

(k, A

F

[2]) classifies the 2-covering Y

αF

−→ A

F

.

X

α

∼ = Kum(Y

αF

) for every quadratic extension F /k. {A

F

}

F/k

- the abelian surfaces associated to X

α

. Diophantine problem of interest

Assuming finiteness of X for all associated abelian surfaces, find

sufficient conditions for the Hasse principle to hold on X

α

.

(17)

Kummer Surfaces

Special case - Kummer surfaces.

k - a number field;

A - an abelian surface over k ;

Y

α

−→ A - a 2-covering, by which we mean a twist of the map A −→

2

A by a class α ∈ H

1

(k, A[2]).

ι : A → A, ι(x) = −x, also acts compatibly on Y

α

;

X

α

= Kum(Y

α

) := the minimal desingularisation of Y

α

/ι, is called the Kummer surface attached to Y

α

.

F /k quadratic ⇒ A

F

[2] ∼ = A[2] and α interpreted in H

1

(k, A

F

[2]) classifies the 2-covering Y

αF

−→ A

F

.

X

α

∼ = Kum(Y

αF

) for every quadratic extension F /k. {A

F

}

F/k

- the abelian surfaces associated to X

α

. Diophantine problem of interest

Assuming finiteness of X for all associated abelian surfaces, find

sufficient conditions for the Hasse principle to hold on X

α

.

(18)

Kummer Surfaces

Special case - Kummer surfaces.

k - a number field;

A - an abelian surface over k ;

Y

α

−→ A - a 2-covering, by which we mean a twist of the map A −→

2

A by a class α ∈ H

1

(k, A[2]).

ι : A → A, ι(x) = −x, also acts compatibly on Y

α

;

X

α

= Kum(Y

α

) := the minimal desingularisation of Y

α

/ι, is called the Kummer surface attached to Y

α

.

F /k quadratic ⇒ A

F

[2] ∼ = A[2] and α interpreted in H

1

(k, A

F

[2]) classifies the 2-covering Y

αF

−→ A

F

.

X

α

∼ = Kum(Y

αF

) for every quadratic extension F /k. {A

F

}

F/k

- the abelian surfaces associated to X

α

. Diophantine problem of interest

Assuming finiteness of X for all associated abelian surfaces, find

sufficient conditions for the Hasse principle to hold on X

α

.

(19)

Kummer Surfaces

Special case - Kummer surfaces.

k - a number field;

A - an abelian surface over k ;

Y

α

−→ A - a 2-covering, by which we mean a twist of the map A −→

2

A by a class α ∈ H

1

(k, A[2]).

ι : A → A, ι(x) = −x, also acts compatibly on Y

α

;

X

α

= Kum(Y

α

) := the minimal desingularisation of Y

α

/ι, is called the Kummer surface attached to Y

α

.

F /k quadratic ⇒ A

F

[2] ∼ = A[2] and α interpreted in H

1

(k, A

F

[2]) classifies the 2-covering Y

αF

−→ A

F

.

X

α

∼ = Kum(Y

αF

) for every quadratic extension F /k. {A

F

}

F/k

- the abelian surfaces associated to X

α

. Diophantine problem of interest

Assuming finiteness of X for all associated abelian surfaces, find

sufficient conditions for the Hasse principle to hold on X

α

.

(20)

Kummer Surfaces

Special case - Kummer surfaces.

k - a number field;

A - an abelian surface over k ;

Y

α

−→ A - a 2-covering, by which we mean a twist of the map A −→

2

A by a class α ∈ H

1

(k, A[2]).

ι : A → A, ι(x) = −x, also acts compatibly on Y

α

;

X

α

= Kum(Y

α

) := the minimal desingularisation of Y

α

/ι, is called the Kummer surface attached to Y

α

.

F /k quadratic ⇒ A

F

[2] ∼ = A[2] and α interpreted in H

1

(k, A

F

[2]) classifies the 2-covering Y

αF

−→ A

F

.

X

α

∼ = Kum(Y

αF

) for every quadratic extension F /k. {A

F

}

F/k

- the abelian surfaces associated to X

α

. Diophantine problem of interest

Assuming finiteness of X for all associated abelian surfaces, find

sufficient conditions for the Hasse principle to hold on X

α

.

(21)

Kummer Surfaces

Special case - Kummer surfaces.

k - a number field;

A - an abelian surface over k ;

Y

α

−→ A - a 2-covering, by which we mean a twist of the map A −→

2

A by a class α ∈ H

1

(k, A[2]).

ι : A → A, ι(x) = −x, also acts compatibly on Y

α

;

X

α

= Kum(Y

α

) := the minimal desingularisation of Y

α

/ι, is called the Kummer surface attached to Y

α

.

F /k quadratic ⇒ A

F

[2] ∼ = A[2] and α interpreted in H

1

(k, A

F

[2]) classifies the 2-covering Y

αF

−→ A

F

.

X

α

∼ = Kum(Y

αF

) for every quadratic extension F /k. {A

F

}

F/k

- the abelian surfaces associated to X

α

. Diophantine problem of interest

Assuming finiteness of X for all associated abelian surfaces, find

sufficient conditions for the Hasse principle to hold on X

α

.

(22)

Kummer Surfaces

Special case - Kummer surfaces.

k - a number field;

A - an abelian surface over k ;

Y

α

−→ A - a 2-covering, by which we mean a twist of the map A −→

2

A by a class α ∈ H

1

(k, A[2]).

ι : A → A, ι(x) = −x, also acts compatibly on Y

α

;

X

α

= Kum(Y

α

) := the minimal desingularisation of Y

α

/ι, is called the Kummer surface attached to Y

α

.

F /k quadratic ⇒ A

F

[2] ∼ = A[2] and α interpreted in H

1

(k, A

F

[2]) classifies the 2-covering Y

αF

−→ A

F

.

X

α

∼ = Kum(Y

αF

) for every quadratic extension F /k.

{A

F

}

F/k

- the abelian surfaces associated to X

α

. Diophantine problem of interest

Assuming finiteness of X for all associated abelian surfaces, find

sufficient conditions for the Hasse principle to hold on X

α

.

(23)

Kummer Surfaces

Special case - Kummer surfaces.

k - a number field;

A - an abelian surface over k ;

Y

α

−→ A - a 2-covering, by which we mean a twist of the map A −→

2

A by a class α ∈ H

1

(k, A[2]).

ι : A → A, ι(x) = −x, also acts compatibly on Y

α

;

X

α

= Kum(Y

α

) := the minimal desingularisation of Y

α

/ι, is called the Kummer surface attached to Y

α

.

F /k quadratic ⇒ A

F

[2] ∼ = A[2] and α interpreted in H

1

(k, A

F

[2]) classifies the 2-covering Y

αF

−→ A

F

.

X

α

∼ = Kum(Y

αF

) for every quadratic extension F /k.

{A

F

}

F/k

- the abelian surfaces associated to X

α

.

Diophantine problem of interest

Assuming finiteness of X for all associated abelian surfaces, find

sufficient conditions for the Hasse principle to hold on X

α

.

(24)

Kummer Surfaces

Special case - Kummer surfaces.

k - a number field;

A - an abelian surface over k ;

Y

α

−→ A - a 2-covering, by which we mean a twist of the map A −→

2

A by a class α ∈ H

1

(k, A[2]).

ι : A → A, ι(x) = −x, also acts compatibly on Y

α

;

X

α

= Kum(Y

α

) := the minimal desingularisation of Y

α

/ι, is called the Kummer surface attached to Y

α

.

F /k quadratic ⇒ A

F

[2] ∼ = A[2] and α interpreted in H

1

(k, A

F

[2]) classifies the 2-covering Y

αF

−→ A

F

.

X

α

∼ = Kum(Y

αF

) for every quadratic extension F /k.

{A

F

}

F/k

- the abelian surfaces associated to X

α

.

Diophantine problem of interest

(25)

Previous results

Skorobogatov & Swinnerton-Dyer (2005) - sufficient conditions when A = E

1

× E

2

and E

1

[2], E

2

[2] have trivial Galois action. X is then a smooth and proper model for y

2

= f (x)g (z) where

deg(f ) = deg(g ) = 4 whose cubic resolvants define E

1

and E

2

.

Skorobogatov & H. (2015) - sufficient conditions when

A = E

1

× E

2

where E

1

[2] and E

2

[2] have full Galois action, and when A = Jac(C ) with C : y

2

= f (x) hyperelliptic, deg(f ) = 5 irreducible separable. X admits an explicit model as a smooth complete intersection of three quadrics in P

5

.

Both results use variants of Swinnerton-Dyer’s method. Pioneered by Swinnerton-Dyer in 1995, established as a general method by Colliot-Th´ el` ene, Skorobogatov and Swinnerton-Dyer (1998), and later extended and simplified by Wittenberg (2007).

Applies in principle to surfaces which are fibered into curves of

genus 1, typically requires the assumption finiteness of X and

Schinzel’s hypothesis (not needed for the Kummer surface variant)

(26)

Previous results

Skorobogatov & Swinnerton-Dyer (2005) - sufficient conditions when A = E

1

× E

2

and E

1

[2], E

2

[2] have trivial Galois action. X is then a smooth and proper model for y

2

= f (x)g (z) where

deg(f ) = deg(g ) = 4 whose cubic resolvants define E

1

and E

2

. Skorobogatov & H. (2015) - sufficient conditions when

A = E

1

× E

2

where E

1

[2] and E

2

[2] have full Galois action, and when A = Jac(C ) with C : y

2

= f (x) hyperelliptic, deg(f ) = 5 irreducible separable. X admits an explicit model as a smooth complete intersection of three quadrics in P

5

.

Both results use variants of Swinnerton-Dyer’s method. Pioneered by Swinnerton-Dyer in 1995, established as a general method by Colliot-Th´ el` ene, Skorobogatov and Swinnerton-Dyer (1998), and later extended and simplified by Wittenberg (2007).

Applies in principle to surfaces which are fibered into curves of

genus 1, typically requires the assumption finiteness of X and

Schinzel’s hypothesis (not needed for the Kummer surface variant)

(27)

Previous results

Skorobogatov & Swinnerton-Dyer (2005) - sufficient conditions when A = E

1

× E

2

and E

1

[2], E

2

[2] have trivial Galois action. X is then a smooth and proper model for y

2

= f (x)g (z) where

deg(f ) = deg(g ) = 4 whose cubic resolvants define E

1

and E

2

. Skorobogatov & H. (2015) - sufficient conditions when

A = E

1

× E

2

where E

1

[2] and E

2

[2] have full Galois action, and when A = Jac(C ) with C : y

2

= f (x) hyperelliptic, deg(f ) = 5 irreducible separable. X admits an explicit model as a smooth complete intersection of three quadrics in P

5

.

Both results use variants of Swinnerton-Dyer’s method.

Pioneered by Swinnerton-Dyer in 1995, established as a general method by Colliot-Th´ el` ene, Skorobogatov and Swinnerton-Dyer (1998), and later extended and simplified by Wittenberg (2007).

Applies in principle to surfaces which are fibered into curves of

genus 1, typically requires the assumption finiteness of X and

Schinzel’s hypothesis (not needed for the Kummer surface variant)

(28)

Previous results

Skorobogatov & Swinnerton-Dyer (2005) - sufficient conditions when A = E

1

× E

2

and E

1

[2], E

2

[2] have trivial Galois action. X is then a smooth and proper model for y

2

= f (x)g (z) where

deg(f ) = deg(g ) = 4 whose cubic resolvants define E

1

and E

2

. Skorobogatov & H. (2015) - sufficient conditions when

A = E

1

× E

2

where E

1

[2] and E

2

[2] have full Galois action, and when A = Jac(C ) with C : y

2

= f (x) hyperelliptic, deg(f ) = 5 irreducible separable. X admits an explicit model as a smooth complete intersection of three quadrics in P

5

.

Both results use variants of Swinnerton-Dyer’s method. Pioneered by Swinnerton-Dyer in 1995, established as a general method by Colliot-Th´ el` ene, Skorobogatov and Swinnerton-Dyer (1998), and later extended and simplified by Wittenberg (2007).

Applies in principle to surfaces which are fibered into curves of

genus 1, typically requires the assumption finiteness of X and

Schinzel’s hypothesis (not needed for the Kummer surface variant)

(29)

Previous results

Skorobogatov & Swinnerton-Dyer (2005) - sufficient conditions when A = E

1

× E

2

and E

1

[2], E

2

[2] have trivial Galois action. X is then a smooth and proper model for y

2

= f (x)g (z) where

deg(f ) = deg(g ) = 4 whose cubic resolvants define E

1

and E

2

. Skorobogatov & H. (2015) - sufficient conditions when

A = E

1

× E

2

where E

1

[2] and E

2

[2] have full Galois action, and when A = Jac(C ) with C : y

2

= f (x) hyperelliptic, deg(f ) = 5 irreducible separable. X admits an explicit model as a smooth complete intersection of three quadrics in P

5

.

Both results use variants of Swinnerton-Dyer’s method. Pioneered by Swinnerton-Dyer in 1995, established as a general method by Colliot-Th´ el` ene, Skorobogatov and Swinnerton-Dyer (1998), and later extended and simplified by Wittenberg (2007).

Applies in principle to surfaces which are fibered into curves of

genus 1, typically requires the assumption finiteness of X and

Schinzel’s hypothesis (not needed for the Kummer surface variant)

(30)

Main result

A - Jacobian of y

2

= f (x) = Q

5

i=0

(x − a

i

).

d := Q

i<j

(a

j

− a

i

) 6= 0.

A[2] = {(ε

0

, ..., ε

5

) ∈ µ

62

0

· ... · ε

6

= 1}/µ

2

H

1

(k, A[2]) ∼ = {(b

0

, ..., b

5

) ∈ G

6

|b

1

· ... · b

5

= 1}/ G ( G := k

/(k

)

2

) For a class b ∈ H

1

(k, A[2]) associated Kummer surface is

X

b

: X

i

b

i

x

i2

f

0

(a

i

) = X

i

b

i

a

i

x

i2

f

0

(a

i

) = X

i

b

i

a

2i

x

i2

f

0

(a

i

) = 0

Theorem (H. 2016)

Let A, {a

i

}, b be as above. Assume that

bb1

0

, ...,

bb4

0

are linearly

independent in G and that for every i = 1, ..., 5 there exists a place

w

i

such that val

wi

(a

i

− a

0

) = val

wi

d = 1 and val

wi

(b

j

/b

0

) = 0.

Assume that the 2-primary torsion subgroup of X is finite for

every quadratic twist of A. Then the BM obstruction is the only

one for the Hasse principle on the Kummer surfaces X

b

.

(31)

Main result

A - Jacobian of y

2

= f (x) = Q

5

i=0

(x − a

i

).

d := Q

i<j

(a

j

− a

i

) 6= 0.

A[2] = {(ε

0

, ..., ε

5

) ∈ µ

62

0

· ... · ε

6

= 1}/µ

2

H

1

(k, A[2]) ∼ = {(b

0

, ..., b

5

) ∈ G

6

|b

1

· ... · b

5

= 1}/ G ( G := k

/(k

)

2

) For a class b ∈ H

1

(k, A[2]) associated Kummer surface is

X

b

: X

i

b

i

x

i2

f

0

(a

i

) = X

i

b

i

a

i

x

i2

f

0

(a

i

) = X

i

b

i

a

2i

x

i2

f

0

(a

i

) = 0

Theorem (H. 2016)

Let A, {a

i

}, b be as above. Assume that

bb1

0

, ...,

bb4

0

are linearly

independent in G and that for every i = 1, ..., 5 there exists a place

w

i

such that val

wi

(a

i

− a

0

) = val

wi

d = 1 and val

wi

(b

j

/b

0

) = 0.

Assume that the 2-primary torsion subgroup of X is finite for

every quadratic twist of A. Then the BM obstruction is the only

one for the Hasse principle on the Kummer surfaces X

b

.

(32)

Main result

A - Jacobian of y

2

= f (x) = Q

5

i=0

(x − a

i

).

d := Q

i<j

(a

j

− a

i

) 6= 0.

A[2] = {(ε

0

, ..., ε

5

) ∈ µ

62

0

· ... · ε

6

= 1}/µ

2

H

1

(k, A[2]) ∼ = {(b

0

, ..., b

5

) ∈ G

6

|b

1

· ... · b

5

= 1}/ G ( G := k

/(k

)

2

) For a class b ∈ H

1

(k, A[2]) associated Kummer surface is

X

b

: X

i

b

i

x

i2

f

0

(a

i

) = X

i

b

i

a

i

x

i2

f

0

(a

i

) = X

i

b

i

a

2i

x

i2

f

0

(a

i

) = 0

Theorem (H. 2016)

Let A, {a

i

}, b be as above. Assume that

bb1

0

, ...,

bb4

0

are linearly

independent in G and that for every i = 1, ..., 5 there exists a place

w

i

such that val

wi

(a

i

− a

0

) = val

wi

d = 1 and val

wi

(b

j

/b

0

) = 0.

Assume that the 2-primary torsion subgroup of X is finite for

every quadratic twist of A. Then the BM obstruction is the only

one for the Hasse principle on the Kummer surfaces X

b

.

(33)

Main result

A - Jacobian of y

2

= f (x) = Q

5

i=0

(x − a

i

).

d := Q

i<j

(a

j

− a

i

) 6= 0.

A[2] = {(ε

0

, ..., ε

5

) ∈ µ

62

0

· ... · ε

6

= 1}/µ

2

H

1

(k, A[2]) ∼ = {(b

0

, ..., b

5

) ∈ G

6

|b

1

· ... · b

5

= 1}/ G ( G := k

/(k

)

2

) For a class b ∈ H

1

(k, A[2]) associated Kummer surface is

X

b

: X

i

b

i

x

i2

f

0

(a

i

) = X

i

b

i

a

i

x

i2

f

0

(a

i

) = X

i

b

i

a

2i

x

i2

f

0

(a

i

) = 0

Theorem (H. 2016)

Let A, {a

i

}, b be as above. Assume that

bb1

0

, ...,

bb4

0

are linearly independent in G and that for every i = 1, ..., 5 there exists a place w

i

such that val

wi

(a

i

− a

0

) = val

wi

d = 1 and val

wi

(b

j

/b

0

) = 0.

Assume that the 2-primary torsion subgroup of X is finite for

every quadratic twist of A. Then the BM obstruction is the only

one for the Hasse principle on the Kummer surfaces X

b

.

(34)

Swinnerton-Dyer’s method for Kummer surfaces

A - an abelian surface with a principal polarization coming from a symmetric line bundle on A.

X

α

= Kum(Y

α

) has points everywhere locally and no Brauer-Manin obstruction.

Step 1: find a quadratic extension F = k ( √

a) such that Y

αF

has points everywhere locally. Replacing Y

α

with Y

αF

we may assume without loss of generality that Y

α

itself has points everywhere locally. In particular, α ∈ Sel

2

(A).

Step 2: find a quadratic extension such that Sel

2

(A

F

) is generated by α and the image of the 2-torsion.

⇒ conclude that X (A

F

)[2] is generated by the image of α. By assumption X (A

F

) is finite and the Cassels-Tate pairing is alternating (Poonen-Stoll) ⇒ the dimension of X (A

F

)[2] is even ⇒ X (A

F

)[2] = 0 ⇒ Y

αF

(k ) 6= ∅ ⇒ X

α

(k) 6= ∅.

Problem

Sometimes step 2 is not possible (without further assumptions)

(35)

Swinnerton-Dyer’s method for Kummer surfaces

A - an abelian surface with a principal polarization coming from a symmetric line bundle on A. X

α

= Kum(Y

α

) has points

everywhere locally and no Brauer-Manin obstruction.

Step 1: find a quadratic extension F = k ( √

a) such that Y

αF

has points everywhere locally. Replacing Y

α

with Y

αF

we may assume without loss of generality that Y

α

itself has points everywhere locally. In particular, α ∈ Sel

2

(A).

Step 2: find a quadratic extension such that Sel

2

(A

F

) is generated by α and the image of the 2-torsion.

⇒ conclude that X (A

F

)[2] is generated by the image of α. By assumption X (A

F

) is finite and the Cassels-Tate pairing is alternating (Poonen-Stoll) ⇒ the dimension of X (A

F

)[2] is even ⇒ X (A

F

)[2] = 0 ⇒ Y

αF

(k ) 6= ∅ ⇒ X

α

(k) 6= ∅.

Problem

Sometimes step 2 is not possible (without further assumptions)

(36)

Swinnerton-Dyer’s method for Kummer surfaces

A - an abelian surface with a principal polarization coming from a symmetric line bundle on A. X

α

= Kum(Y

α

) has points

everywhere locally and no Brauer-Manin obstruction.

Step 1: find a quadratic extension F = k ( √

a) such that Y

αF

has points everywhere locally. Replacing Y

α

with Y

αF

we may assume without loss of generality that Y

α

itself has points everywhere locally. In particular, α ∈ Sel

2

(A).

Step 2: find a quadratic extension such that Sel

2

(A

F

) is generated by α and the image of the 2-torsion.

⇒ conclude that X (A

F

)[2] is generated by the image of α. By assumption X (A

F

) is finite and the Cassels-Tate pairing is alternating (Poonen-Stoll) ⇒ the dimension of X (A

F

)[2] is even ⇒ X (A

F

)[2] = 0 ⇒ Y

αF

(k ) 6= ∅ ⇒ X

α

(k) 6= ∅.

Problem

Sometimes step 2 is not possible (without further assumptions)

(37)

Swinnerton-Dyer’s method for Kummer surfaces

A - an abelian surface with a principal polarization coming from a symmetric line bundle on A. X

α

= Kum(Y

α

) has points

everywhere locally and no Brauer-Manin obstruction.

Step 1: find a quadratic extension F = k ( √

a) such that Y

αF

has points everywhere locally. Replacing Y

α

with Y

αF

we may assume without loss of generality that Y

α

itself has points everywhere locally. In particular, α ∈ Sel

2

(A).

Step 2: find a quadratic extension such that Sel

2

(A

F

) is generated by α and the image of the 2-torsion.

⇒ conclude that X (A

F

)[2] is generated by the image of α. By assumption X (A

F

) is finite and the Cassels-Tate pairing is alternating (Poonen-Stoll) ⇒ the dimension of X (A

F

)[2] is even ⇒ X (A

F

)[2] = 0 ⇒ Y

αF

(k ) 6= ∅ ⇒ X

α

(k) 6= ∅.

Problem

Sometimes step 2 is not possible (without further assumptions)

(38)

Swinnerton-Dyer’s method for Kummer surfaces

A - an abelian surface with a principal polarization coming from a symmetric line bundle on A. X

α

= Kum(Y

α

) has points

everywhere locally and no Brauer-Manin obstruction.

Step 1: find a quadratic extension F = k ( √

a) such that Y

αF

has points everywhere locally. Replacing Y

α

with Y

αF

we may assume without loss of generality that Y

α

itself has points everywhere locally. In particular, α ∈ Sel

2

(A).

Step 2: find a quadratic extension such that Sel

2

(A

F

) is generated by α and the image of the 2-torsion.

⇒ conclude that X (A

F

)[2] is generated by the image of α.

By assumption X (A

F

) is finite and the Cassels-Tate pairing is alternating (Poonen-Stoll) ⇒ the dimension of X (A

F

)[2] is even ⇒ X (A

F

)[2] = 0 ⇒ Y

αF

(k ) 6= ∅ ⇒ X

α

(k) 6= ∅.

Problem

Sometimes step 2 is not possible (without further assumptions)

(39)

Swinnerton-Dyer’s method for Kummer surfaces

A - an abelian surface with a principal polarization coming from a symmetric line bundle on A. X

α

= Kum(Y

α

) has points

everywhere locally and no Brauer-Manin obstruction.

Step 1: find a quadratic extension F = k ( √

a) such that Y

αF

has points everywhere locally. Replacing Y

α

with Y

αF

we may assume without loss of generality that Y

α

itself has points everywhere locally. In particular, α ∈ Sel

2

(A).

Step 2: find a quadratic extension such that Sel

2

(A

F

) is generated by α and the image of the 2-torsion.

⇒ conclude that X (A

F

)[2] is generated by the image of α.

By assumption X (A

F

) is finite and the Cassels-Tate pairing is alternating (Poonen-Stoll) ⇒ the dimension of X (A

F

)[2] is even ⇒ X (A

F

)[2] = 0 ⇒ Y

αF

(k ) 6= ∅ ⇒ X

α

(k) 6= ∅.

Problem

Sometimes step 2 is not possible (without further assumptions)

(40)

Extending the method

Step 2: find a quadratic extension such that Sel

2

(A

F

) is generated by α and the image of the 2-torsion.

Step 3: find a quadratic extension such that the subgroup Sel

2

(A

F

) ⊆ Sel

2

(A

F

) generated by those elements which are orthogonal to all of Sel

2

(A) with respect to Cassels-Tate pairing is generated by α and the image of the 2-torsion. Assume WLOG that this holds already for A itself.

⇒ conclude that the subgroup X

⊆ X [2] generated by those elements which are orthogonal to X [2] is generated by the image of α. By assumption X (A) is finite and the Cassels-Tate pairing is alternating ⇒ the dimension of X

∼ = X (A)[4]/ X (A)[2] is even

⇒ X

= 0 ⇒ Y

αF

(k ) 6= ∅ ⇒ X

α

(k) 6= ∅.

(41)

Extending the method

Step 2: find a quadratic extension such that Sel

2

(A

F

) is generated by α, the image of the 2-torsion, and a small subgroup of “unavoidable elements”.

Step 3: find a quadratic extension such that the subgroup Sel

2

(A

F

) ⊆ Sel

2

(A

F

) generated by those elements which are orthogonal to all of Sel

2

(A) with respect to Cassels-Tate pairing is generated by α and the image of the 2-torsion. Assume WLOG that this holds already for A itself.

⇒ conclude that the subgroup X

⊆ X [2] generated by those elements which are orthogonal to X [2] is generated by the image of α. By assumption X (A) is finite and the Cassels-Tate pairing is alternating ⇒ the dimension of X

∼ = X (A)[4]/ X (A)[2] is even

⇒ X

= 0 ⇒ Y

αF

(k ) 6= ∅ ⇒ X

α

(k) 6= ∅.

(42)

Extending the method

Step 2: find a quadratic extension such that Sel

2

(A

F

) is generated by α, the image of the 2-torsion, and a small subgroup of “unavoidable elements”.

Step 3: find a quadratic extension such that the subgroup Sel

2

(A

F

) ⊆ Sel

2

(A

F

) generated by those elements which are orthogonal to all of Sel

2

(A) with respect to Cassels-Tate pairing is generated by α and the image of the 2-torsion.

Assume WLOG that this holds already for A itself.

⇒ conclude that the subgroup X

⊆ X [2] generated by those elements which are orthogonal to X [2] is generated by the image of α. By assumption X (A) is finite and the Cassels-Tate pairing is alternating ⇒ the dimension of X

∼ = X (A)[4]/ X (A)[2] is even

⇒ X

= 0 ⇒ Y

αF

(k ) 6= ∅ ⇒ X

α

(k) 6= ∅.

(43)

Extending the method

Step 2: find a quadratic extension such that Sel

2

(A

F

) is generated by α, the image of the 2-torsion, and a small subgroup of “unavoidable elements”.

Step 3: find a quadratic extension such that the subgroup Sel

2

(A

F

) ⊆ Sel

2

(A

F

) generated by those elements which are orthogonal to all of Sel

2

(A) with respect to Cassels-Tate pairing is generated by α and the image of the 2-torsion.

Assume WLOG that this holds already for A itself.

⇒ conclude that the subgroup X

⊆ X [2] generated by those elements which are orthogonal to X [2] is generated by the image of α. By assumption X (A) is finite and the Cassels-Tate pairing is alternating ⇒ the dimension of X

∼ = X (A)[4]/ X (A)[2] is even

⇒ X

= 0 ⇒ Y

αF

(k ) 6= ∅ ⇒ X

α

(k) 6= ∅.

(44)

The second step

F /k - a quadratic extension. M := A[2] ∼ = A

F

[2].

For v a place - W

v

, W

vF

⊆ H

1

(k

v

, M) the images of A(k

v

), and A

F

(k

v

).

Note dim

2

W

v

= dim

2

W

vF

= 4 =

12

dim

2

H

1

(k

v

, M ).

Goal

Compare the groups

Sel

2

(A) = {β ∈ H

1

(k, M)| loc

v

(β) ∈ W

v

}

Sel

2

(A

F

) = {β ∈ H

1

(k, M )| loc

v

(β) ∈ W

vF

}

(45)

The second step

F /k - a quadratic extension.

M := A[2] ∼ = A

F

[2].

For v a place - W

v

, W

vF

⊆ H

1

(k

v

, M) the images of A(k

v

), and A

F

(k

v

).

Note dim

2

W

v

= dim

2

W

vF

= 4 =

12

dim

2

H

1

(k

v

, M ).

Goal

Compare the groups

Sel

2

(A) = {β ∈ H

1

(k, M)| loc

v

(β) ∈ W

v

}

Sel

2

(A

F

) = {β ∈ H

1

(k, M )| loc

v

(β) ∈ W

vF

}

(46)

The second step

F /k - a quadratic extension.

M := A[2] ∼ = A

F

[2].

For v a place - W

v

, W

vF

⊆ H

1

(k

v

, M) the images of A(k

v

), and A

F

(k

v

).

Note dim

2

W

v

= dim

2

W

vF

= 4 =

12

dim

2

H

1

(k

v

, M ).

Goal

Compare the groups

Sel

2

(A) = {β ∈ H

1

(k, M)| loc

v

(β) ∈ W

v

}

Sel

2

(A

F

) = {β ∈ H

1

(k, M )| loc

v

(β) ∈ W

vF

}

(47)

The second step

F /k - a quadratic extension.

M := A[2] ∼ = A

F

[2].

For v a place - W

v

, W

vF

⊆ H

1

(k

v

, M) the images of A(k

v

), and A

F

(k

v

).

Note dim

2

W

v

= dim

2

W

vF

= 4 =

12

dim

2

H

1

(k

v

, M ).

Goal

Compare the groups

Sel

2

(A) = {β ∈ H

1

(k, M)| loc

v

(β) ∈ W

v

}

Sel

2

(A

F

) = {β ∈ H

1

(k, M )| loc

v

(β) ∈ W

vF

}

(48)

The second step

F /k - a quadratic extension.

M := A[2] ∼ = A

F

[2].

For v a place - W

v

, W

vF

⊆ H

1

(k

v

, M) the images of A(k

v

), and A

F

(k

v

).

Note dim

2

W

v

= dim

2

W

vF

= 4 =

12

dim

2

H

1

(k

v

, M ).

Goal

Compare the groups

Sel

2

(A) = {β ∈ H

1

(k, M )| loc

v

(β) ∈ W

v

}

Sel

2

(A

F

) = {β ∈ H

1

(k , M )| loc

v

(β ) ∈ W

vF

}

(49)

Comparing Selmer groups

Compare the groups

Sel

2

(A) = {β ∈ H

1

(k, M)| loc

v

(β) ∈ W

v

} Sel

F2

(A) = {β ∈ H

1

(k, M)| loc

v

(β) ∈ W

vF

}

T - the (finite) set of places where W

v

6= W

vF

.

W

v

:= W

v

/(W

v

∩ W

vF

) and W

Fv

:= W

vF

/(W

v

∩ W

vF

). r

v

:= dim

2

W

v

= dim

2

W

Fv

.

V

T

⊆ ⊕

v∈T

W

Fv

- the image of Sel

2

(A). V

TF

⊆ ⊕

v∈T

W

Fv

- the image of Sel

2

(A

F

).

dim

2

Sel

2

(A

F

) − dim

2

Sel

2

(A) = dim

2

V

TF

− dim

2

V

T

. Lemma (Mazur-Rubin)

dim

2

V

T

+ dim

2

V

TF

≤ X

v∈T

r

v

(50)

Comparing Selmer groups

Compare the groups

Sel

2

(A) = {β ∈ H

1

(k, M)| loc

v

(β) ∈ W

v

} Sel

F2

(A) = {β ∈ H

1

(k, M)| loc

v

(β) ∈ W

vF

} T - the (finite) set of places where W

v

6= W

vF

.

W

v

:= W

v

/(W

v

∩ W

vF

) and W

Fv

:= W

vF

/(W

v

∩ W

vF

). r

v

:= dim

2

W

v

= dim

2

W

Fv

.

V

T

⊆ ⊕

v∈T

W

Fv

- the image of Sel

2

(A). V

TF

⊆ ⊕

v∈T

W

Fv

- the image of Sel

2

(A

F

).

dim

2

Sel

2

(A

F

) − dim

2

Sel

2

(A) = dim

2

V

TF

− dim

2

V

T

. Lemma (Mazur-Rubin)

dim

2

V

T

+ dim

2

V

TF

≤ X

v∈T

r

v

(51)

Comparing Selmer groups

Compare the groups

Sel

2

(A) = {β ∈ H

1

(k, M)| loc

v

(β) ∈ W

v

} Sel

F2

(A) = {β ∈ H

1

(k, M)| loc

v

(β) ∈ W

vF

}

T - the (finite) set of places where W

v

6= W

vF

.

W

v

:= W

v

/(W

v

∩ W

vF

) and W

Fv

:= W

vF

/(W

v

∩ W

vF

).

r

v

:= dim

2

W

v

= dim

2

W

Fv

.

V

T

⊆ ⊕

v∈T

W

Fv

- the image of Sel

2

(A). V

TF

⊆ ⊕

v∈T

W

Fv

- the image of Sel

2

(A

F

).

dim

2

Sel

2

(A

F

) − dim

2

Sel

2

(A) = dim

2

V

TF

− dim

2

V

T

. Lemma (Mazur-Rubin)

dim

2

V

T

+ dim

2

V

TF

≤ X

v∈T

r

v

(52)

Comparing Selmer groups

Compare the groups

Sel

2

(A) = {β ∈ H

1

(k, M)| loc

v

(β) ∈ W

v

} Sel

F2

(A) = {β ∈ H

1

(k, M)| loc

v

(β) ∈ W

vF

}

T - the (finite) set of places where W

v

6= W

vF

.

W

v

:= W

v

/(W

v

∩ W

vF

) and W

Fv

:= W

vF

/(W

v

∩ W

vF

).

r

v

:= dim

2

W

v

= dim

2

W

Fv

.

V

T

⊆ ⊕

v∈T

W

Fv

- the image of Sel

2

(A). V

TF

⊆ ⊕

v∈T

W

Fv

- the image of Sel

2

(A

F

).

dim

2

Sel

2

(A

F

) − dim

2

Sel

2

(A) = dim

2

V

TF

− dim

2

V

T

. Lemma (Mazur-Rubin)

dim

2

V

T

+ dim

2

V

TF

≤ X

v∈T

r

v

(53)

Comparing Selmer groups

Compare the groups

Sel

2

(A) = {β ∈ H

1

(k, M)| loc

v

(β) ∈ W

v

} Sel

F2

(A) = {β ∈ H

1

(k, M)| loc

v

(β) ∈ W

vF

}

T - the (finite) set of places where W

v

6= W

vF

.

W

v

:= W

v

/(W

v

∩ W

vF

) and W

Fv

:= W

vF

/(W

v

∩ W

vF

).

r

v

:= dim

2

W

v

= dim

2

W

Fv

.

V

T

⊆ ⊕

v∈T

W

Fv

- the image of Sel

2

(A).

V

TF

⊆ ⊕

v∈T

W

Fv

- the image of Sel

2

(A

F

).

dim

2

Sel

2

(A

F

) − dim

2

Sel

2

(A) = dim

2

V

TF

− dim

2

V

T

. Lemma (Mazur-Rubin)

dim

2

V

T

+ dim

2

V

TF

≤ X

v∈T

r

v

(54)

Comparing Selmer groups

Compare the groups

Sel

2

(A) = {β ∈ H

1

(k, M)| loc

v

(β) ∈ W

v

} Sel

F2

(A) = {β ∈ H

1

(k, M)| loc

v

(β) ∈ W

vF

}

T - the (finite) set of places where W

v

6= W

vF

.

W

v

:= W

v

/(W

v

∩ W

vF

) and W

Fv

:= W

vF

/(W

v

∩ W

vF

).

r

v

:= dim

2

W

v

= dim

2

W

Fv

.

V

T

⊆ ⊕

v∈T

W

Fv

- the image of Sel

2

(A).

V

TF

⊆ ⊕

v∈T

W

Fv

- the image of Sel

2

(A

F

).

dim

2

Sel

2

(A

F

) − dim

2

Sel

2

(A) = dim

2

V

TF

− dim

2

V

T

. Lemma (Mazur-Rubin)

dim

2

V

T

+ dim

2

V

TF

≤ X

v∈T

r

v

(55)

Comparing Selmer groups

Compare the groups

Sel

2

(A) = {β ∈ H

1

(k, M)| loc

v

(β) ∈ W

v

} Sel

F2

(A) = {β ∈ H

1

(k, M)| loc

v

(β) ∈ W

vF

}

T - the (finite) set of places where W

v

6= W

vF

.

W

v

:= W

v

/(W

v

∩ W

vF

) and W

Fv

:= W

vF

/(W

v

∩ W

vF

).

r

v

:= dim

2

W

v

= dim

2

W

Fv

.

V

T

⊆ ⊕

v∈T

W

Fv

- the image of Sel

2

(A).

V

TF

⊆ ⊕

v∈T

W

Fv

- the image of Sel

2

(A

F

).

dim

2

Sel

2

(A

F

) − dim

2

Sel

2

(A) = dim

2

V

TF

− dim

2

V

T

.

Lemma (Mazur-Rubin)

dim

2

V

T

+ dim

2

V

TF

≤ X

v∈T

r

v

(56)

Comparing Selmer groups

Compare the groups

Sel

2

(A) = {β ∈ H

1

(k, M)| loc

v

(β) ∈ W

v

} Sel

F2

(A) = {β ∈ H

1

(k, M)| loc

v

(β) ∈ W

vF

}

T - the (finite) set of places where W

v

6= W

vF

.

W

v

:= W

v

/(W

v

∩ W

vF

) and W

Fv

:= W

vF

/(W

v

∩ W

vF

).

r

v

:= dim

2

W

v

= dim

2

W

Fv

.

V

T

⊆ ⊕

v∈T

W

Fv

- the image of Sel

2

(A).

V

TF

⊆ ⊕

v∈T

W

Fv

- the image of Sel

2

(A

F

).

dim

2

Sel

2

(A

F

) − dim

2

Sel

2

(A) = dim

2

V

TF

− dim

2

V

T

.

Lemma (Mazur-Rubin)

(57)

Comparing Selmer groups (continuation)

Mazur-Rubin Lemma dim

2

V

T

+ dim

2

V

TF

≤ P

v∈T

r

v

Proof.

The Weil pairing induces the non-degenerate local Tate pairing

∪ : H

1

(k

v

, M) × H

1

(k

v

, M ) −→ H

2

(k

v

, µ

2

) = Z /2 with W

v

and W

vF

maximal isotropic.

Restricting to W

v

× W

vF

, summing over v ∈ T and dividing by W

v

∩ W

vF

yields

non-degenerate pairing

v∈T

W

v

× ⊕

v∈T

W

Fv

−→ Z /2 between two vector spaces of dimension r = P

v∈T

r

v

. Quadratic reciprocity ⇒ V

T

⊆ ⊕

v∈T

W

v

is orthogonal to V

TF

⊆ ⊕

v∈T

W

Fv

and hence the sum of their dimensions cannot accede r

(gap is

even by Poonen-Rains).

(58)

Comparing Selmer groups (continuation)

Mazur-Rubin Lemma dim

2

V

T

+ dim

2

V

TF

≤ P

v∈T

r

v

Proof.

The Weil pairing induces the non-degenerate local Tate pairing

∪ : H

1

(k

v

, M) × H

1

(k

v

, M ) −→ H

2

(k

v

, µ

2

) = Z /2 with W

v

and W

vF

maximal isotropic.

Restricting to W

v

× W

vF

, summing over v ∈ T and dividing by W

v

∩ W

vF

yields

non-degenerate pairing

v∈T

W

v

× ⊕

v∈T

W

Fv

−→ Z /2 between two vector spaces of dimension r = P

v∈T

r

v

. Quadratic reciprocity ⇒ V

T

⊆ ⊕

v∈T

W

v

is orthogonal to V

TF

⊆ ⊕

v∈T

W

Fv

and hence the sum of their dimensions cannot accede r

(gap is

even by Poonen-Rains).

(59)

Comparing Selmer groups (continuation)

Mazur-Rubin Lemma dim

2

V

T

+ dim

2

V

TF

≤ P

v∈T

r

v

Proof.

The Weil pairing induces the non-degenerate local Tate pairing

∪ : H

1

(k

v

, M) × H

1

(k

v

, M ) −→ H

2

(k

v

, µ

2

) = Z /2 with W

v

and W

vF

maximal isotropic. Restricting to W

v

× W

vF

, summing over v ∈ T and dividing by W

v

∩ W

vF

yields

non-degenerate pairing

v∈T

W

v

× ⊕

v∈T

W

Fv

−→ Z /2 between two vector spaces of dimension r = P

v∈T

r

v

. Quadratic reciprocity ⇒ V

T

⊆ ⊕

v∈T

W

v

is orthogonal to V

TF

⊆ ⊕

v∈T

W

Fv

and hence the sum of their dimensions cannot accede r.

(gap is

even by Poonen-Rains).

(60)

Comparing Selmer groups (continuation)

Mazur-Rubin Lemma dim

2

V

T

+ dim

2

V

TF

≤ P

v∈T

r

v

Proof.

The Weil pairing induces the non-degenerate local Tate pairing

∪ : H

1

(k

v

, M) × H

1

(k

v

, M ) −→ H

2

(k

v

, µ

2

) = Z /2 with W

v

and W

vF

maximal isotropic. Restricting to W

v

× W

vF

, summing over v ∈ T and dividing by W

v

∩ W

vF

yields

non-degenerate pairing

v∈T

W

v

× ⊕

v∈T

W

Fv

−→ Z /2 between two vector spaces of dimension r = P

v∈T

r

v

. Quadratic

reciprocity ⇒ V

T

⊆ ⊕

v∈T

W

v

is orthogonal to V

TF

⊆ ⊕

v∈T

W

Fv

(61)

Examples

Assume M = A[2] has constant Galois action.

Example (Selmer stays the same)

T = {v

0

, v

1

} and dim

2

W

v0

= dim

2

W

v1

= 4. Then dim

2

V

T

+ dim

2

V

TF

≤ 8.

dim

2

V

T

, dim

2

V

TF

≥ 4 ⇒ dim

2

Sel

2

(A

F

) = dim

2

Sel

2

(A).

Example (Selmer decreases)

T = {w , v

0

, v

1

}, dim

2

W

v0

= dim

2

W

v1

= 4 and dim

2

W

w

= 1. dim

2

V

T

+ dim

2

V

TF

≤ 8 + 1 = 9.

dim

2

V

T

≥ 5 ⇒ dim

2

Sel

2

(A

F

) ≤ dim

2

Sel

2

(A) − 1.

(62)

Examples

Assume M = A[2] has constant Galois action.

Example (Selmer stays the same)

T = {v

0

, v

1

} and dim

2

W

v0

= dim

2

W

v1

= 4. Then dim

2

V

T

+ dim

2

V

TF

≤ 8.

dim

2

V

T

, dim

2

V

TF

≥ 4 ⇒ dim

2

Sel

2

(A

F

) = dim

2

Sel

2

(A).

Example (Selmer decreases)

T = {w , v

0

, v

1

}, dim

2

W

v0

= dim

2

W

v1

= 4 and dim

2

W

w

= 1. dim

2

V

T

+ dim

2

V

TF

≤ 8 + 1 = 9.

dim

2

V

T

≥ 5 ⇒ dim

2

Sel

2

(A

F

) ≤ dim

2

Sel

2

(A) − 1.

(63)

Examples

Assume M = A[2] has constant Galois action.

Example (Selmer stays the same)

T = {v

0

, v

1

} and dim

2

W

v0

= dim

2

W

v1

= 4. Then dim

2

V

T

+ dim

2

V

TF

≤ 8.

dim

2

V

T

, dim

2

V

TF

≥ 4 ⇒ dim

2

Sel

2

(A

F

) = dim

2

Sel

2

(A).

Example (Selmer decreases)

T = {w , v

0

, v

1

}, dim

2

W

v0

= dim

2

W

v1

= 4 and dim

2

W

w

= 1. dim

2

V

T

+ dim

2

V

TF

≤ 8 + 1 = 9.

dim

2

V

T

≥ 5 ⇒ dim

2

Sel

2

(A

F

) ≤ dim

2

Sel

2

(A) − 1.

(64)

Examples

Assume M = A[2] has constant Galois action.

Example (Selmer stays the same)

T = {v

0

, v

1

} and dim

2

W

v0

= dim

2

W

v1

= 4. Then dim

2

V

T

+ dim

2

V

TF

≤ 8.

dim

2

V

T

, dim

2

V

TF

≥ 4 ⇒ dim

2

Sel

2

(A

F

) = dim

2

Sel

2

(A).

Example (Selmer decreases)

T = {w , v

0

, v

1

}, dim

2

W

v0

= dim

2

W

v1

= 4 and dim

2

W

w

= 1.

dim

2

V

T

+ dim

2

V

TF

≤ 8 + 1 = 9.

dim

2

V

T

≥ 5 ⇒ dim

2

Sel

2

(A

F

) ≤ dim

2

Sel

2

(A) − 1.

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