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Notes on class field theory

Section 7.1 Cohomology of the idèles I: the “First Inequality”

Reference.

[37] VII.2-VII.4; [38] VI.3, but see below. See also this blog post by Akhil Mathew
 1 
amathew.wordpress.com/2010/05/30/the-first-inequality-cohomology-of-the-idele-classes/
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By analogy with local class field theory, we want to prove that for L/K a cyclic extension of number fields and CK,CL the respective idèle class groups of K and L,
H1(Gal(L/K),CL)=1,H2(Gal(L/K),CL)=Z/[L:K]Z.
Our first step is to calculate the Herbrand quotient (in analogy with Proposition 4.2.11).

Proof.

This will end up reducing to a study of lattices in a real vector space, much as in the proof of Dirichlet’s units theorem (Corollary 6.2.11).
From Theorem 7.1.1, we will deduce the so-called “First Inequality”.

Proof.

The “Second Inequality” will be the reverse, which will be a bit more subtle (see Theorem 7.2.9).

Subsection Some basic observations

Definition 7.1.3. Notational shorthand.

Let L/K be a Galois extension of number fields with Galois group G. (We do not yet need G to be cyclic.) For any finite set S of places of K containing all infinite places, write IL,S to mean the group IL,T where T denotes the set of places of L lying over some place in S. Similarly, write oL,S to mean oL,T.
Note that each IL,S is stable under the action of G and that IL is the direct limit of the IL,S over all S. Moreover, by Corollary 6.2.10, for S sufficiently large we have
IL=IL,SL.

Proof.

The group Hi(G,IL,S) is the product of Hi(G,w|vLw) over all vS and Hi(G,w|voLw) over all vS. By Shapiro’s lemma (Lemma 3.2.3), we may reinterpret Hi(G,IL,S) as the product of Hi(Gw,Lw) over all vS and Hi(Gw,oLw) over all vS. The latter vanish for all i>0 by Corollary 4.2.6, so we get what we want. The argument for Tate groups is analogous.

Proof.

View IL as the direct limit of the IL,S over all finite sets S of places of K containing all infinite places and all ramified places; then Hi(G,IL) is the direct limit of the Hi(G,IL,S). We may thus apply Proposition 7.1.4 to deduce the claims.

Proof.

Remark 7.1.7. Sanity check.

The case of HT0 in Corollary 7.1.5 asserts something that is evidently true and already featured in the proof of Lemma 6.4.1: an idèle in IK is a norm from IL if and only if each component is a norm.

Subsection Cohomology of the units: first steps

Definition 7.1.8.

Let L/K be a cyclic extension of number fields with Galois group G. Apply Corollary 6.2.10 to choose a finite set S of places of K, containing all infinite places and all places which ramify in L, such that IL=IL,SL. From the exact sequence
1oL,SIL,SIL,S/oL,S=CL1
we have an equality of Herbrand quotients
h(CL)=h(IL,S)/h(oL,S).
h(IL,S)=vS[Lw:Kv].
To get h(CL)=[L:K], it will thus suffice to establish Lemma 7.1.9 below.

Proof.

Subsection Cohomology of the units: a computation with S-units

At this point, we have reduced the computation of the Herbrand quotient h(IL), and by extension the First Inequality, to the computation of h(oL,S) for a suitable set S of places of K. We treat this point next, using similar ideas to the proof of Dirichlet’s units theorem (Corollary 6.2.11).

Definition 7.1.10.

Let L/K be a cyclic extension of number fields with Galois group G. Let S be a finite set of places of K containing all infinite places, and let T be the set of places of L lying above places of S. Let V be the real vector space consisting of one copy of R for each place in T. Define the map oL,SV by
αwTlog|α|w
with normalizations as in Definition 6.1.11. By the product formula (Proposition 6.1.12) and Dirichlet’s units theorem (Corollary 6.2.11), the kernel of this map consists of roots of unity, and the image M is a lattice in the trace-zero hyperplane H of V. Since G acts compatibly on oL,S and V (the latter by permuting the factors), it also acts on M.

Remark 7.1.11. Caveat.

At this point, we deviate from [38] due to an error therein. Namely, Lemma VI.3.4 is only proved assuming that G acts transitively on the coordinates of V, but in Definition 7.1.10 this is not the case: G permutes the places above any given place v of K but those are separate orbits. So we’ll follow [37] instead.

Definition 7.1.12.

Continuing from Definition 7.1.10, we can write down two natural lattices in V. One of them is the lattice generated by M together with the all-ones vector, on which G acts trivially. As a G-module, the Herbrand quotient of that lattice is h(M)h(Z)=[L:K]h(M). The other is the lattice M in which, in the given coordinate system, each element has integral coordinates. To compute the Herbrand quotient of M, notice that the projection of this lattice onto the coordinates corresponding to the places wT above some vS form a copy of IndGvGZ. Writing h(G,) for the Herbrand quotient to emphasize the dependence on the group G, we have
h(G,M)=vSh(G,IndGvGZ)=vSh(Gv,Z)=vS#Gv=vS[Lw:Kv].
To sum up, the calculations from Definition 7.1.10 and Definition 7.1.12 reduce Lemma 7.1.9 to a comparison of Herbrand quotients of two lattices in the same real vector space. See Lemma 7.1.13.

Subsection Herbrand quotients of real lattices

We conclude the proof of the First Inequality with the following statement.

Proof.

Note that L1ZQ and L2ZQ are Q[G]-modules which become isomorphic to V, and hence to each other, after tensoring over Q with R. By Lemma 7.1.14, this implies that L1ZQ and L2ZQ are isomorphic as Q[G]-modules.
From this isomorphism, we see that as a Z[G]-module, L1 is isomorphic to some sublattice of L2. Since a lattice has the same Herbrand quotient as any sublattice (the quotient is finite, so its Herbrand quotient is 1 by Remark 3.4.8), that means h(L1)=h(L2).

Proof.

By hypothesis, the F-vector space
WF:=HomF(V1EF,V2EF),
on which G acts by the formula Tg(x)=T(xg1)g, contains an invariant vector which, as a linear transformation, is invertible. Now WF can also be written as
WEF,W:=HomE(V1,V2).
The fact that WF has an invariant vector says that a certain set of linear equations has a nonzero solution over F, namely the equations that express the fact that the action of G leaves the vector invariant. But those equations have coefficients in E, so
WGEF=WFG;
in particular, the space of invariant vectors in W is also nonzero.
It remains to check that some element of WG corresponds to a map V1V2 which is actually an isomorphism; for this, we argue as in Exercise 3. Fix an isomorphism of vector spaces between V2EF and V1EF (which need not respect the G-action). By composing each element of W with this isomorphism and taking the determinant, we get a well-defined polynomial function on W, which we can restrict to WG. By hypothesis, this function is not identically zero on WFG, so (because E is infinite) it cannot be identically zero on WG either.

Subsection Splitting of primes

As a consequence of the First Inequality, we record the following fact which was previously stated as a consequence of the Chebotaryov density theorem (Theorem 2.4.11), but which will be needed logically earlier in the arguments. (See [38], Corollary VI.3.8 for more details.) Alternatively, we will get something stronger out of the analytic proof of the Second Inequality (Proposition 7.2.3).

Proof.

Suppose first that L/K is cyclic. Suppose that all but finitely many primes split completely; we can then take a finite set S of places which contains all of them as well as all of the infinite places and all of the ramified places. For each vS, the group Uv:=NormLw/KvLw is open of finite index in Kv. For any αIK, using the approximation theorem (Proposition 6.1.18) we can then find βK such that (α/β)vUv for all vS. For each place vS, we have Lw=Kv, so α/βNormL/KIL. We deduce that the class of α in CL is a norm; that is, CK=NormL/KCL, whereas Theorem 7.1.2 asserts that HT0(Gal(L/K),CL)[L:K], contradiction.
In the general case, let M be the Galois closure of L/K; then a prime of K splits completely in L if and only if it splits completely in M. Since Gal(M/K) is a nontrivial finite group, it contains a cyclic subgroup; let N be the fixed field of this subgroup. By the previous paragraph, there are infinitely many prime ideals of N which do not split completely in M, proving the original result.

Exercises Exercises

1.

Let K be a number field. Let L1,,Lr be cyclic extensions of K of the same prime degree p such that LiLj=K for ij. Using the First Inequality (Theorem 7.1.2), prove that there are infinitely many primes of K which split completely in L2,,Lr but not in L1.