Euler Systems
1 Heegner points (and BSD) 1.1 Introduction Let be an elliptic curve over , ∼ r(E,F ). E Q [F : Q] < ∞ ⇒ E(F ) = E(F )tor ⊗ Z Q −s −1 Q −s 1−2s −1 Given E, we have an L-function, L(E, s) = (1 − app ) (1 − app + p ) with Re(s) > 3/2 p|N p-N p + 1 − #E(Fp) p - N 0 E additive at p and ap = , N = cond(E). 1 split multi at p −1 non split multi at p Q Q p Q p Note. L(E, 1) ” = ” () · = where Np = #E( p)ns. p|N p-N p−ap+1 p Np F Conjecture (Birch-Swinnerton-Dyer). Let E/Q be an elliptic curve 1. ords=1L(E, s) = rkZE(Q) = r
2. L(E,s) det(hPi,Pj i) Q , where are generators of . lims→1 r = #X(E, Q) 2 v|N cv {Pi} E(Q) (s−1) #E(Q)tor
Suppose that E is modular (now we know this is always true): there exists f ∈ S2(Γ0(N)) a newform f(q) = P∞ n such that P∞ −s. Or equivalently . This implies that n=1 anq L(E, s) = L(f, s) = n=1 ann ap(E) = ap(f) L(E, s) has analytic continuation to C. It has a functorial equation ∧(E, s) = (2π)−sΓ(s)N s/2L(E, s). We have ∧(E, s) = − ∧ (E, 2 − s) where ∈ {±1} and is determined by wN (f) = · f where w is the Atkin-Lehner function. We shall call − the sign(E, Q). modular representation. non-constant morphism dened over . f φ : X0(N)/Q / E/Q Q O Hecke−op AJ ( J0(N) = JacX0(N)
1.2 Class eld theory Let be an imaginary quadratic eld. Let be an order, , an integer. K ⊆ C On ⊆ K On = Z + nOK n ≥ 1 ∼ By class eld theory: There is a map rec : Pic(On) = Gal(Kn/K) where Kn/K is an abelian extension unramied away from n. Recall that Pic(On) = I(n)/P (n) where I(n) = {fractional ideals coprime to n}, P (n) = . The map is dened by −1 h(α): α ∈ OK , α ≡ a mod nOK , a ∈ Zi [p] 7→ Frobp Lemma. Let . Then ∼ ∼ ∗ ∗. In particular, if is Gn = Gal(Kn/K1) Gn = Pic(On)/Pic(OK ) = (OK /nOK ) / (Z/nZ) ` ( ` + 1 ` inert in K an odd prime unramied in K, then G` is cyclic and [K` : K1] = ` − 1 ` split in K If is square free then ∼ Q . n Gn = `|n G`
1 1.3 Complex Multiplication
0 0 X0(N) classies (up to isomorphism) cyclic N-isogonies, A → A where ker(A → A ) is cyclic of order N. Let imaginary eld satisfying Heegner Hypothesis: splits in . Can pick an ideal such that K/Q `|N ⇒ ` K N ⊆ OK ∼ (cyclic). Consider , −1 where OK /N = Z/NZ On = Z + nOK χn = [C/On → C/Nn ] ∈ X0(N)(C) Nn = N ∩ On ( ∼ ). ⇒ On/Nn = Z/NZ Theorem (Main Theorem of Complex Multiplication). Let ∼ so σ ∈ Aut(C/K) σ|Kn ∈ Gal(Kn/K) = Pic(On) . σ|Kn [aσ] σ −1 −1 −1 χn = C/aσ → C/Nn aσ Remark. Suppose . Then σ . Hence . σ|Kn = 1 χn = χn χn ∈ X0(N)(Kn) Hecke action (On ): For each , is a correspondence on χ0(N) ` - N T` X0(N) T` : (DivX0(N))(F ) → dened by 0 P 0 . DivX0(N)(F ) [φ : A 7→ A ] 7→ C⊂A[`],cyclic subgp of order `[A/C → A /φ(C)] Also have the Trace map: Tr` : DivX0(N)(Kn`) → DivX0(N)(Kn). Proposition. Consider , where . Let , then {χn}n (n, ND) = 1 D = disc(K) ` - ND T χ if ` n is inert in K ` n - 1. As elements in , −1 DivX0(N)(Kn) Tr`(χn`) = (T` − Frobλ − Frobλ )χn if ` = λλ - n split in K T`χn − χn/` `|n
2. If is inert in , , is a prime in above . Then Frobλn ` - N K λ = `OK λn Kn λ redλn` (χn`) = redλn (χn ) ∈ . X0(N)(Fλn )
1.4 Heegner points on E
Let φ : X0(N) → E. yn := φ(χn) is the Heegner point of conductor n (in E(Kn)). (in ) is the basis Heegner point yK = TrK1/K (y1) E(K) Proposition. ` - ND : a y if ` is inert in K, ` n ` n - −1 Frobλn Tr`(yn`) = (a` − Frobλ − Frobλ )yn redλn`(yn`) = redλn(yn ) a`yn − yn/` E(Fλn ) Proposition. If is a complex conjugation, then there exists such that τ σ on τ σ ∈ Gal(Kn/K) yn = yn E(K)/E(K)tors .
2 Local Cohomology 2.1 Introduction to cohomology
Let G be a group and M a G-module. Both G and M have topology. 1-cocycles: Are {f : G → M|f continuous and ∀g, h ∈ G, f(gh) = f(g) + gf(h)} 1-coboundary: Are {f : G → M|f continuous and f(g) = g · m − m for some m ∈ M} Denition 2.1. H1(G, M) ={1-cocylce}/{1-coboundary}, H0(G, M) = M G Consider the short exact sequence of G-modules, 0 → M 0 → M → M 00 → 0 and M 00 → M is a continuous section of sets. Then we get a long exact sequence
0 → M 0G → M G → M 00G → H1(G, M 0) → H1(G, M) → H1(G, M 00) → H2 ... We have some useful maps between cohomology groups:
2 • Let H ≤ G, we get a map Res : H1(G, M) → H1(H,M).
1 H 1 • Let H C G be a normal closed subgroup of G, then we have inf : H (G/H, M ) → H (G, M) We have the following relationship between inf and Res called the Hochschild-Serre spectral sequence
0 → H1(G/H, M H ) →inf H1(G, M) Res→ H1(H,M)G/H → H2(G/H, M H ) → ...
2.2 Galois Cohomology Fox prime , and and let un be the maximal unramied extension of and let un ` p |K : Q`| < ∞ K K IK = Gal(K/K ) be the Inertia group Denote by and un un ∼ (∼ ) GK = Gal(K/K) GK = Gal(K /K) = GK /IK = Zb Let be a nite dimensional -vector space with discrete action. We say that is unramied if acts T Fp GK T IK trivially on T . 1 1 ∗ ∗ There is a perfect pairing of -vector spaces where ∞ . Fp H (GK ,T ) ⊗Fp H (GK ,T ) → Fp T = Hom(T,Mp ) Fact. If and is unramied then 1 un and 1 un ∗ are exact orthogonal complements with respect ` 6= p T H (GK ,T ) H (GK ,T ) to h , i. Denition 2.2. A local Selmer structure for is a choice of -subspace of 1 denoted 1 . F T Fp H (GK ,T ) Hf,F (GK ,T ) We call the quotient 1 1 1 the singular quotient. HS,F (GK ,T ) := H (GK ,T )/Hf,F (GK ,T )
1 1 1 0 → Hf,F (GK ,T ) → H (GK ,T ) → HS,F (GK ,T ) → 0 (†)
We say is an unramied structure if 1 1 un IK (via inf). In this case identies with inf-res. F Hf,F (GK ,T ) = H (GK ,T ) (†) Using the Tate pairing we dene the Dual Selmer structure F ∗ on T ∗ to be the exact orthogonal complement of 1 . Hf,F (GK ,T ) 1 ∗ In particular ∗ we get an induced perfect pairing. HS,F (GK ,T ) ⊗Fp Hf,F (GK ,T ) → Fp 2.3 Local cohomology for elliptic curves Let be an elliptic curve over . We let . We have the Weil pairing E K T = E[p] = E(K)[P ] E[P ] ⊗ FpE[P ] → µp ∗ ∼ (⇒ E[P ] = E[P ]). We have a short exact sequence of GK -module
p 0 → E[P ] → E(K) → E(K) → 0
If we take the associated long exact sequence
GK GK GK 1 1 0 → E[P ] → E(K) → E(K) → H (GK ,E[P ]) → H (GK ,E(K)) → ... (††)
From (††) we get: δ 1 1 0 → E(K)/pE(K) → H (GK ,E[p]) → H (GK ,E(K))[p] → 0 where δ is dened as follows: for Q ∈ E(K) x L ∈ E(K) such that pL = Q. Then δ(Q) is the 1-cocycle which sends σ ∈ GK to σ(L) − L ∈ E[P ].
1 Denition 2.3. The geometric local Selmer structure F on E[P ] is the image of δ in H (GK ,E[p]). Fact. The dual geometric local Selmer structure is the geometric local Selmer structure (it make sense since E[P ]∗ =∼ E[P ]) If E has good reduction over K and ` 6= p. Then E[p] is an unramied GK -module and the geometric structures agrees with the unramied structure.
3 3 Global Section
In this talk K will be a number eld, v a place of K, Kv the completion of K at v, Gv = Gal(Kv/Kv) and Iv the inertia subgroup of . As in the last talk we let to be a nite dimensional -vector space with a discrete Gv T Fp GK -action. GK × T → T is continuous when T is given the discrete topology. We choose an embedding K,→ Kv which gives us an embedding Gv ,→ GK . Since T is nite dimensional and GK acts discretely, this implies that T is unramied almost everywhere. 1 1 For each place v we have a restriction map Resv : H (K,T ) → H (Kv,T ).
3.1 Selmer Groups Denition 3.1. A global Selmer structure on is a choice of a local Selmer structure 1 for each F T Hf,F (Kv,T ) place such that 1 1 unr Iv almost everywhere. v Hf,F (Kv,T ) = H (Kv ,T ) The Selmer group of is dened to be 1 1 . SelF (K,T ) F ker H (K,T ) → ⊕vHs,F (Kv,T ) If we take E to be an elliptic curve over K and T = E[p]. Denition 3.2. The geometric global Selmer structure F on E[p] is dened to be the global Selmer structure obtained by setting 1 to be the local geometric structure at each . Hf,F (Kv,T ) v (p) In this setting SelF (K,E[p]) = Sel (E).
3.2 Global Duality
Denition 3.3. Let F be a global Selmer structure on T . The Cartier dual Selmer structure F ∗ on T ∗ = is dened to be the global Selmer structure obtained by setting 1 ∗ to be the local Cartier HomFp (T, µp) Hf,F ∗ (Kv,T ) dual Selmer structure. We now x an F and F ∗ and start omitting it from notation. Given an ideal , we dene 1 1 for all . a C OK Sela(K,T ) = {c ∈ H (K,T ): cv ∈ Hf,F (Kv,T ) v - a} a Sel (K,T ) = {c ∈ SelF (K,T ): cv = 0, ∀v|a}. This gives us the following exact sequences 1 0 → Sel(K,T ) → Sela(K,T ) → ⊕v|aHS,F (Kv,T ) → 0
a ∗ ∗ 1 ∗ 0 → Sel (K,T ) → Sel(K,T ) → ⊕v|aHf,F (Kv,T ) → 0 We have 1 ∼ 1 ∗ ∨. We can put the two sequences above together as follows ⊕v|aHs,F (Kv,T ) = ⊕v|aHf,F ∗ (Kv,T )
M 1 ∗ ∨ a ∗ ∨ 0 → Sel(K,T ) → Sela(K,T ) → Hs,F (K,T ) → Sel(K,T ) → Sel (K,T ) → 0 v|a Proposition 3.4. The above sequence is exact. The exactness of this sequence yields