This paper extends arithmetic Chern-Simons theory to include number fields with real places and constructs new non-trivial invariants with non-abelian gauge groups, broadening the scope of previous models.
Contribution
It generalizes arithmetic Chern-Simons theory to arbitrary number fields with real places and provides new non-trivial examples with non-abelian gauge groups and general coefficients.
Findings
01
Extended theory to include real places using cohomology with compact support.
02
Constructed new non-trivial invariants with non-abelian gauge groups.
03
Provided explicit examples via a twisting argument.
Abstract
The goal of this paper is two-fold: we generalize the arithmetic Chern-Simons theory over totally imaginary number fields studied in [Kim15, CKK+16] to arbitrary number fields (with real places) and provide new examples of non-trivial arithmetic Chern-Simons invariant with coefficient Z/nZ(n≥2) associated to a non-abelian gauge group. The main idea for the generalization is to use cohomology with compact support (see [Mil06]) to deal with real places. Before the results of this paper, non-trivial examples were limited to some non-abelian gauge group with coefficient Z/2Z in [CKK+16] and the abelian cyclic gauge group with coefficient Z/nZ in [BCG+18]. Our non-trivial examples (with non-abelian gauge group and general coefficient Z/nZ) will be given by a simple twisting argument based on examples of…
No public reviews on file for this paper yet. If you reviewed it on a platform where reviews are public (OpenReview, ICLR, NeurIPS, ICML), you can paste yours below so the community can read it here.
Videos
No videos yet. Explain this paper in a talk, walkthrough, or lecture? Add one.
Taxonomy
TopicsBlack Holes and Theoretical Physics · Noncommutative and Quantum Gravity Theories · Advanced Operator Algebra Research
Full text
ARITHMETIC CHERN-SIMONS THEORY WITH REAL PLACES
JUNGIN LEE, JEEHOON PARK
Abstract
The goal of this paper is two-fold: we generalize the arithmetic Chern-Simons
theory over totally imaginary number fields studied in [Kim15, CKK+16] to arbitrary number fields (with real places) and provide
new examples of non-trivial arithmetic Chern-Simons invariant with coefficient
Z/nZ(n≥2) associated to a non-abelian gauge group.
The main idea for the generalization is to use cohomology with compact support (see [Mil06]) to deal with real places. Before the results of this paper, non-trivial examples were limited to some non-abelian gauge group with coefficient Z/2Z in [CKK+16] and the abelian cyclic gauge group with coefficient Z/nZ in [BCG+18].
Our non-trivial examples (with non-abelian gauge group and general coefficient Z/nZ) will be given by a simple twisting argument based on examples of [BCG+18].
Arithmetic topology is an area which studies an analogy between knots in 3-manifold theory and primes in number theory, based on homotopical analogies between them. Such an analogy was first suggested in the 1960’s by B. Mazur. Later, M. Kapranov [Kap96] and A. Reznikov [Rez97] examined the analogy further and proved some interesting results. It was M. Morishita who studied arithmetic topology more systematically in his series of papers including [Mor02],[Mor04]; he also published a wonderful book [Mor12] on the subject.
Chern-Simons theory is a 3-dimensional topological quantum field theory with gauge group.
It has been used to understand knot invariants such as the Jones polynomial.
Then the analogy between knots and primes (arithmetic topology) leads to a question whether there is an arithmetic analogue of Chern Simon theory which can be used to understand number-theoretic invariants further.
It was Minhyong Kim (see [Kim15]) who answered this question when the gauge group is finite (also suggested a way to define the theory when the gauge group is a p-adic analytic group).
He defined the arithmetic Chern-Simons action (also called the arithmetic Chern-Simons invariant) by applying the ideas of Dijkgraaf and Witten (see [DW90]) on a 3-dimensional topological quantum field theory to an arithmetic curve, namely the spectrum of the ring of integers in an algebraic number field. Then, in [CKK+16], H. Chung, D. Kim, M. Kim, H. Yoo together with the second-named author continued to study the theory to provide non-trivial examples of the arithmetic Chern-Simons functional. Also, an intimate connection between the abelian arithmetic Chern-Simons theory and arithmetic linking numbers of prime ideals (number-theoretic invariants) is investigated in [CKK+19].
Let us briefly recall the setting of [Kim15, CKK+16]. Let F be a totally imaginary number field and OF the ring of integers of F.
Let X=Spec(OF) and n≥2 be a natural number.
Assume that F contains a primitive n-th roots of unity.
Then there is a canonical isomorphism
[TABLE]
Denote πun:=Gal(Fun/F) where Fun is the maximal unramified extension of F in an algebraic closure F.
Let A be a finite group (called the gauge group).
Consider the space of fields on the space time X:
[TABLE]
where A acts on the target by conjugation.
Fix a group cohomology class c∈H3(A,Z/nZ) where A acts on Z/nZ trivially.
Define the arithmetic classical Chern-Simons action (or invariant) without boundary by the function
[TABLE]
where jun3:H3(πun,Z/nZ)→H3(X,Z/nZ) is the edge map
induced from the Hochschild-Serre spectral sequence (see (2) for an alternative precise definition of jun3).
Since ρ∗(c) depends only on the class [ρ], CSc is well-defined.
A technical reason why F is assumed to be totally imaginary in [Kim15, CKK+16]
is that the isomorphism (1) does not hold anymore when F has a real place.
A natural idea for generalizing the arithmetic Chern-Simons theory to an arbitrary
number field is to use cohomology with compact support, since there is a canonical isomorphism
(see Proposition 2.4)
[TABLE]
for any number field F containing a primitive n-th roots of unity.
Based on this isomorphism, we extend the arithmetic classical Chern-Simons action without boundary to an arbitrary number field.
Since we assume that F contains a primitive n-th roots of unity111If n≥3 under this assumption, then F is totally imaginary., the actual new case
compared to [CKK+16] is that n=2 and F is a real number field.
But we will state propositions and theorems for arbitrary number fields F and natural numbers n for efficiency of the presentation of proofs and examples.
Let Sf be any finite set of finite primes of F,
X∞ be the set of all real places of F,
S:=Sf∪X∞,
S be any set satisfying Sf⊂S⊂S,
US:=Spec(OF[Sf1]) and
πS:=Gal(FunS/F) where FunS is the maximal extension of F in F unramified outside S.
When working with the arithmetic classical Chern-Simons action with boundary (see (5))
and proving the decomposition formula222This provides a way of computing the arithmetic classical Chern-Simons action without boundary using a comparison between local unramified and global ramified trivializations of a Galois three cocycle. (see Section 3),
the vanishing of the étale cohomology group H3(USf,Z/nZ) plays an important role.
Another key difference between totally imaginary fields and real number fields lies in the vanishing behavior of H3. If Sf contains places of F above n, then H3(USf,Z/nZ)=0 for an arbitrary number field F but H3(US~,Z/nZ)=0 for a real field F and S~ which strictly includes Sf.
Due to this difference, our Chern-Simons action and decomposition formula differ from those in [CKK+16].
In Section 5, [CKK+16], the authors used the decomposition formula to construct infinitely many totally imaginary number fields F in which the action CSc([ρ]) is non-zero for some c and ρ when n=2 and the gauge group A is Z/2Z,Z/2Z×Z/2Z, or the symmetric group S4.
We provide analogues of those examples for the totally real case.
In Section 6, [CKK+16], they showed non-solvability of a certain case of the embedding problem (biquadratic fields are involved) based on non-vanishing ([CKK+16, Theorem 6.2]) of the arithmetic Chern-Simons action with gauge group V4, the Klein four group. Unfortunately, such an arithmetic application is not available in our case with totally real fields.
An example of non-vanishing of CSc([ρ]) for the case n>2 but with the abelian cyclic gauge group A=Z/nZ was first provided by the work of F. M. Bleher, T. Chinburg, R. Greenberg, M. Kakde, G. Pappas and M. J. Taylor, in [BCG+18].
When A=Z/nZ for any n≥2, they found infinitely many totally imaginary number fields F and representations
ρ such that CSc([ρ])=0 for a choice of c (see [BCG+18, Theorem 1.2]).
Here we prove that there are infinitely many totally imaginary number fields F such that CSc([ρ])=0 for some ρ and c, when the gauge group is A=G⋊Z/nZ (the semidirect product of some finite group G by Z/nZ) for any n≥2 (See Lemma 4.21 and Theorem 4.22.) For instance, we will give examples of non-vanishing arithmetic Chern-Simons action
(see Example 4.24) where the gauge group is the general linear group GL(r,Fp) over the finite field Fp (r≥2) and n=p−1.
There exists the method of Zink [Zin78] and Conrad-Masullo [CM] of generalizing the étale cohomology of X=Spec(OF) for totally imaginary number fields F, which was studied by Mazur [Maz73], to arbitrary number fields.
This provides an alternative way of defining the arithmetic classical Chern-Simons action. In the appendix, we add such a viewpoint. Note that the approach based on cohomology with compact support has a benefit of providing a natural framework to prove the decomposition formula.
The methods of this paper using cohomology with compact support carry over mutatis mutandis to the case of global function fields provided n is prime to the characteristic of the field. So there is also a version of
arithmetic Chern-Simons theory for a finite extension F of the field of rational functions Fp(T) when n is prime to a prime number p.
We briefly explain the contents of each section. In Section 2.1, we set up basic definitions
and notations. In Section 2.2 we review the theory of cohomology with compact support based on Milne’s book [Mil06]. We define the arithmetic classical Chern-Simons action without boundary (in Section 2.3) and with boundary (in Section 2.4). Since we do not deal with the quantization of the theory and we will omit the word “classical” in the body of the paper. Section 3 is devoted to a statement and a proof of the decomposition formula.
Section 4 is about examples. We provide analogous examples to Section 5, [CKK+16] (in Section 4.1) and to Section 6, [CKK+16] (in Section 4.2)
in the case of totally real number fields with the coefficient Z/2Z and the gauge group A=Z/2Z,Z/2Z×Z/2Z, or S4.
In Section 4.3, we provide non-vanishing examples with general n and some non-abelian gauge group based on the result of [BCG+18]. Finally, we add an alternative viewpoint of the arithmetic Chern-Simons theory with real places based on the generalized étale cohomology theory developed by Zink and Conrad-Masullo.
2 Arithmetic Chern-Simons action
In this section, we define the arithmetic Chern-Simons action for an arbitrary number field. To deal with the real places of a number field F, we use cohomologies with compact support.
2.1 Definitions and notations
Let F be a number field, X=Spec(OF), GF:=Gal(F/F), b:Spec(F)→X be a geometric point and π:=π1(X,b).
Then π≅Gal(Funf/F) where Funf is the maximal extension of F in F unramified at all finite primes.
Denote πun:=Gal(Fun/F) where Fun is the maximal unramified extension of F in F.
Let Sf be any finite set of finite primes of F,
X∞ be the set of all real places of F,
S:=Sf∪X∞,
S be any set satisfying Sf⊂S⊂S,
US:=Spec(OF[Sf1]) and
bS:Spec(F)→US be a geometric point and
πS:=Gal(FunS/F) where FunS is the maximal extension of F in F unramified outside S.
Then π1(US,bS)≅πS.
Let pS:πS→πSf and κS:πS→πun be natural quotient maps. For each (possibly infinite) prime v of F, let πv:=Gal(Fv/Fv), Iv⊂πv be the inertia group and
κv:πv→GF→πun
be given by choices of embeddings F→Fv.
For each v∈S, let
iv=iv,S:πv→GF→πS be given by the embeddings F→Fv same as above and iv′=iv,S′:Spec(Fv)→Spec(F)→US be the natural map.
For a πS-module M, let Mv be M equipped with the πv-module structure given by iv. Similarly, for an abelian étale sheaf F on US, denote the abelian étale sheaf on Spec(Fv) induced by iv′ by Fv. For a finite abelian group G, its Pontryagin dual GD:=Hom(G,Q/Z) is isomorphic to G. For a Galois group G=Gal(L/K) and a G-module M, denote the dual group of M by M∨:=HomG(M,L×). For a locally constant abelian étale sheaf F on US, its Cartier dual F∨:=HomUS(F,Gm) is also locally constant and F∨∨≅F.
2.2 Cohomology with compact support
We write rv for the restriction map of cochains or cohomology classes from πS~ to πv (induced by iv) or from US to Spec(Fv) (induced by iv′). Since the category of abelian étale sheaves on Spec(Fv) is equivalent to the category of πv-modules ([Fu11, Proposition 5.7.8]), the second map can be also viewed as the map of cochains or cohomology classes from US to πv.
Let C(G,M) be the standard inhomogeneous group cochain complex of a group G with values in M. For any finite πS-module M, we consider the complex defined as a mapping fiber:
[TABLE]
and
[TABLE]
Explicitly,
[TABLE]
and d(a,(bv)v∈S)=(da,(rv(a)−dbv)v∈S) for (a,(bv)v∈S)∈Ccn(πS,M). By the definition of Hcr(πS,M), there is a long exact sequence
[TABLE]
For an abelian étale sheaf F on US, the complex
[TABLE]
and
[TABLE]
are defined by the same way and the same long exact sequence holds.
Proposition 2.1**.**
([Mil06, Proposition 2.2.6]) Hc2(US,Gm)=0, Hc3(US,Gm)=Q/Z and Hcr(US,Gm)=0 for all r>3.
Remark 2.2**.**
([Mil06, Remark 2.2.8(a)]) Let OF×,+ be the group of totally positive units of F, and Cl+(F) be the narrow class group of F. Then Hc0(X,Gm)=OF×,+ and Hc1(X,Gm)=Cl+(F).
Theorem 2.3**.**
([Mil06, Theorem 2.3.1]; Artin-Verdier duality) Let F be a constructible sheaf on an open subscheme U of X. The Yoneda pairing
[TABLE]
is a nondegenerate pairing of finite abelian groups for all r∈Z.
For an abelian group A, let AUS be the constant sheaf on the étale site Et(US) (defined in Section 2.2) defined by A.
Proposition 2.4**.**
Hc3(US,Z/nZ)≅μn(F)D.
Proof.
By Artin-Verdier duality,
[TABLE]
The isomorphism (Z/nZ)US∨≅ker(ZUS∨→nZUS∨)=ker(Gm,US→nGm,US)=μn,US implies
[TABLE]
Denote the isomorphism Hc3(US,Z/nZ)→μn(F)D by invS and Hc3(X,Z/nZ)→μn(F)D by inv. Note that the following diagram commutes and the map Hc3(X,Z/nZ)→Hc3(US,Z/nZ) is an isomorphism.
[TABLE]
2.3 Arithmetic Chern-Simons action without boundary
Let FSetπS be the category of finite continuous πS-sets, FEt(US) be the category of finite étale US-schemes and Et(US) be the category of étale US-schemes.
Each category can be understood as a site with a natural Grothendieck topology.
Since the functor FEt(US)→FSetπS (Y↦Y(bS):=HomUS(Spec(F),Y)) is an equivalence of categories ([Fu11, Theorem 3.2.12]) and there is a natural morphism of sites FEt(US)→Et(US), the map
[TABLE]
is defined and it induces a homomorphism
[TABLE]
It is easy to show that the map H3(πun,Z/nZ)→Hc3(π,Z/nZ) given by
[TABLE]
is a well-defined group homomorphism.
(Note that κX∞:π≅Gal(Funf/F)→πun=Gal(Fun/F) is the natural quotient map, i.e. κX∞ is the map κS defined in Section 2.1 for Sf=ϕ and S=X∞.)
Now define the map jun3 by
[TABLE]
Let A be a finite group, M(A):=Homcont(πun,A)/A and fix a class c∈H3(A,Z/nZ) for an integer n≥2. Define the arithmetic Chern-Simons action by a function
[TABLE]
Since ρ∗(c) depends only on the class [ρ], CSc is well-defined.
Proposition 2.5**.**
Let m>0 be a divisor of n such that μn(F)=μm(F) (for example, m=∣μn(F)∣), α:Z/nZ→Z/mZ be the group homomorphism defined by α(1)=1 and c′=α∗c∈H3(A,Z/mZ). Then CSc([ρ])=CSc′([ρ]) for every [ρ]∈M(A).
Proof.
The proposition follows from the following commutative diagram.
[TABLE]
∎
By the proposition above, we may assume that μn(F)=μn(F) which we assume from now on. Since F is totally imaginary for n≥3 under this assumption, the case n=2 is the only case which [CKK+16] does not cover.
Note that there is an isomorphism between μn(F)D with n1Z/Z so that we can regard CSc a n1Z/Z-valued function.
Later when we state and prove the decomposition formula, we will choose an identification ϕ:μn(F)D∼n1Z/Z (see (2), Section 3).
2.4 Arithmetic Chern-Simons action with boundary
Let Sn be any finite set of finite primes of F containing primes of F above n. Denote T=Sn∪X∞ and Tf=Sn. Note that T=Tf=Sn for n≥3 due to the assumption μn(F)=μn(F).
For T′∈{T,Tf}, let
[TABLE]
equipped with the conjugation action of A and denote its action groupoid by MT′(A).
Similarly, let
[TABLE]
equipped with the conjugation action of AT′:=∏v∈T′A and denote its action groupoid by MT′loc(A).
Define the functor rT′:MT′(A)→MT′loc(A) by
[TABLE]
Let CTi:=∏v∈TCi(πv,Z/nZ),
ZTi:=∏v∈TZi(πv,Z/nZ) and
BTi:=∏v∈TBi(πv,Z/nZ) be the product of continuous cochains, cocycles and coboundaries for each v∈T and dT:=(dv)v∈T:CT2→ZT3. Let ρT:=(ρv)v∈T∈YTloc(A), c∘ρT:=(c∘ρv)v∈T and c∘Ada:=(c∘Adav)v∈T for a=(av)v∈T∈AT where Adav:A→A is defined by Adav(x)=avxav−1. For HT2:=∏v∈TH2(πv,Z/nZ),
[TABLE]
is a HT2-torsor.
By [Ser97, Theorem 2.5.2], there is an isomorphism invv:H2(πv,Z/nZ)→n1Z/Z for all v∈T. By the Poitou-Tate exact sequence ([Mil06, Theorem I.4.10]), the sequence
[TABLE]
is exact. Denote the map HT2→H0(πT,Z/nZ∨)D≃n1Z/Z by ∑ and let
[TABLE]
be the n1Z/Z-torsor defined by the pushout of the HT2-torsor H(ρT) by ∑.
By [NSW, Proposition 8.3.18] and [NSW, Theorem 10.6.1], H3(πTf,Z/nZ)=0 so for ρ∈YTf(A), c∘ρ=dβ for some β∈C2(πTf,Z/nZ). Then for the quotient map pT:πT→πTf, we have c∘ρ∘pT=d(β∘pT) and d(iT∗(β∘pT))=c∘iT∗(ρ∘pT) so [iT∗(β∘pT)]∈H(iT∗(ρ∘pT)). Now define the arithmetic Chern-Simons action with boundary Tf by
[TABLE]
For β,β′∈C2(πTf,Z/nZ) such that dβ=dβ′=c∘ρ, β′=β+z for some z∈Z2(πTf,Z/nZ). Then ∑∗([iT∗(z∘pT)])=0 by the Poitou-Tate exact sequence (3), so CSTf,c is well-defined.
Because H3(πT,Z/nZ)=0 when X∞ is not empty (i.e. there is a real place in F), the arithmetic CS action with boundary does not seem to extend from YTf(A) to YT(A).
Remark 2.6**.**
The map HT2→H0(πT,Z/nZ∨)D is the dual of H0(πT,Z/nZ∨)→∏v∈TH0(πv,Z/nZ∨) induced by iv,T for each v∈T. (Each map corresponds to the map γ2 and β0 in
[Mil06, Theorem I.4.10], respectively. In [Mil06], the map γr is defined to be the dual of β2−r for each r∈Z.)
For each v∈T, the map
H0(πT,Z/nZ∨)→H0(πv,Z/nZ∨) is identified with an isomorphism μn(F)→μn(Fv) so the map ∑ is same as ∑v∈Tinvv and equals to the sum map ∑ of [CKK+16, p. 3].
Note that LT in (4) can be extended to a functor from MTloc(A) to the category of n1Z/Z-torsors Tors(n1Z/Z) exactly as in [CKK+16, p. 6-7].
Denote
[TABLE]
According to the axioms of topological field theory, it is natural to expect that CSTf,c(⋅) is an invariant section of the functor LTglob∘pT∗ (where pT∗:MTf(A)→MT(A) is induced from pT); we provide such a result.
Lemma 2.7**.**
Let ρ∈YT(A) and a∈Aut(ρ) be a morphism in MT(A). Then LTglob(a)=idLTglob(ρ).
Proof.
By the definition of the action groupoid MT(A), Ada∘ρ=ρ. By [CKK+16, Lemma A.2], there is ha∈C2(A,Z/nZ)/B2(A,Z/nZ) such that
[TABLE]
so dha∘ρ=d(ha∘ρ)=0 and ha∘ρ∈H2(πT,Z/nZ). LTglob(a) maps an element of LTglob(ρ) represented by (f,x)∈H(rT(ρ))×n1Z/Z to an element represented by (f+(ha∘ρ∘iv)v∈T,x), or equivalently, (f,x+∑((ha∘ρ∘iv)v∈T)). By the exact sequence (3) above, ∑((ha∘ρ∘iv)v∈T)=0 so LTglob(a) is the identity map on LTglob(ρ).
∎
By the above lemma, LTglob restricted on the orbit [ρ]∈MT(A)=YT(A)/A is a functor from a connected groupoid to Tors(n1Z/Z) with no holonomy. Therefore, the set LTinv([ρ]) of its invariant sections becomes a non-zero n1Z/Z-torsor and it is given explicitly by
[TABLE]
Thus, for a given [ρ]∈MTf(A)=YTf(A)/A, we have [pT∗(ρ)]=[ρ∘pT]∈MT(A) and LTinv([ρ∘pT]) is a n1Z/Z-torsor;
one can check the desired result
[TABLE]
3 Decomposition formula
An explicit computation of the arithmetic Chern-Simons invariant relies on the decomposition formula, which expresses the arithmetic Chern-Simons invariant as the difference of a ramified global trivialization and an unramified local trivialization. In this section, we prove the decomposition formula. The proof is done in several steps.
(1) By [NSW, 8.6.10 (ii)], H3(πT,Z/nZ)≅∏v∈TH3(πv,Z/nZ) so the top row of the following diagram is exact. Its bottom row is exact by Poitou-Tate exact sequence and Remark 2.6.
[TABLE]
From the diagram above, we obtain an isomorphism invT′:Hc3(πT,Z/nZ)→n1Z/Z which makes the diagram commute.
(2) By [CM, Theorem 6.1.1], jc3:Hc3(πT,Z/nZ)→Hc3(UT,Z/nZ) is an isomorphism. Now let ϕ:μn(F)D→n1Z/Z be the isomorphism defined by the composition
[TABLE]
Then the following diagram commutes:
[TABLE]
(3) By [Ser97, Proposition 2.18], H2(πv/Iv,Z/nZ)=H3(πv/Iv,Z/nZ)=0 for every v∈T. Let T1⊂T2 be finite sets of primes of F which may or may not contain real places and denote the projection πT2→πT1 by κT1,T2. The map Hc3(πT1,Z/nZ)→Hc3(πT2,Z/nZ) can be described as follows.
Choose an element [(a,(bv)v∈T1)]∈Hc3(πT1,Z/nZ). For v∈T2∖T1, κv factors through πv/Iv so rv(a) can be restricted to rv(a)∣πv/Iv∈Z3(πv/Iv,Z/nZ)=B3(πv/Iv,Z/nZ). Now there is a canonical
[TABLE]
such that dbv=rv(a)∣πv/Iv. This can be lifted to a canonical class bv∈C2(πv,Z/nZ)/B2(πv,Z/nZ). (Note that bv=0 if v∈X∞.) Now [(κT1,T2∗(a),(bv)v∈T2)] is an element of Hc3(πT2,Z/nZ) and it is independent of the choice of bv because H2(πv/Iv,Z/nZ)=0. The canonical map
[TABLE]
is a group homomorphism and one can deduce that it is same as the map induced by C3(πT1,Z/nZ)→C3(πT2,Z/nZ) from the definition of the mapping fiber.
(4) Let w be the cocycle representing ρ∗(c)∈H3(πun,Z/nZ). By the vanishing of H3(πTf,Z/nZ), we can find a global cochain b+′∈C2(πTf,Z/nZ) such that κTf∗(w)=db+′ (here κTf:πTf→πun is the natural quotient). Denote b+:=b+′∘pT∈C2(πT,Z/nZ) and b+,v:=rv(bv)∈C2(πv,Z/nZ).
From the discussion in (3), the image of ρ∗(c)=[w] in Hc3(πT,Z/nZ) is [(κT∗(w),(b−,v)v∈T)], where b−,v is a lift of b−,v∈C2(πv/Iv,Z/nZ) such that κv∗(w)∣πv/Iv=db−,v. Now
[TABLE]
and by the diagram in (2) and the fact that b−,v=b+,v=0 for v∈X∞,
[TABLE]
Theorem 3.1**.**
Let F be a number field and n≥2 be an integer. For any finite set Tf of finite primes of F containing all primes dividing n with the notations above, we have the decomposition formula
[TABLE]
Proof.
For βv:=b−,v, ∑v∈T(βv):=∑∗((βv)v∈T)∈LTinv([ρ∘κT])
is well-defined and CSTf,c([ρ∘κTf]) is also an element of a n1Z/Z-torsor LTinv([ρ∘κT]) so their difference is an element of n1Z/Z.
It is easy to show that CSTf,c([ρ∘κTf])=∑∗((b+,v)v∈T) and
[TABLE]
4 Examples
In this section, we compute the arithmetic Chern-Simons invariants in certain cases.
In the first 2 subsections, we concentrate on the case n=2 and provide some explicit examples of the computation of CSc([ρ]).
In the last subsection, we prove that for n≥2 and a finite group G, there are infinitely many number fields F whose arithmetic Chern-Simons invariants associated to the gauge group A=G⋊Z/nZ (the semidirect product of G by Z/nZ) are non-vanishing, which generalizes the result of [BCG+18].
4.1 The totally real analogue with n=2
Since most of the results in this section are analogues to Section 5 of [CKK+16], proofs are generally omitted there.
Under the assumption μn(F)=μn(F), (5.1)-(5.5) of [CKK+16] can be extended to every number field F.
Since we use πun rather than π, Assumption 5.7 and 5.9 of [CKK+16] should be refined by adding conditions about unramifiedness at real places.
Assumption 4.1**.**
(1) c=α∪ϵ∈H3(A,Z/2Z) with surjective α:A→Z/2Z, and ϵ∈H2(A,Z/2Z) corresponding to a central extension
[TABLE]
(2) There are Galois extensions of F:
[TABLE]
*such that Gal(F−/F)≅A, Gal(F+/F)≅Γ, F−/F is unramified at all primes (including real primes) and F+/F is unramified at the primes above 2.
(3) Fα is the fixed field of the kernel of the composition Gal(F−/F)≃A→αZ/2Z.
(4) ρ:πun→A is given by the composition πun→Gal(F−/F)≃A, where πun→Gal(F−/F) is the natural projection map.*
Remark 4.2**.**
Let B={F1,⋯,Fm} be the set of subfields of F− which are quadratic extensions of F. Then B is in bijection with the set of surjective homomorphisms Gal(F−/F)→Z/2Z. So for each Fi∈B, there is a unique surjective homomorphism αi:Gal(F−/F)→Z/2Z such that Fαi=Fi.
Let Sf be the set of finite primes of F ramified in F+, S2 be the set of primes of F above 2 (Sf∩S2=ϕ by the assumption) and Tf:=Sf∪S2. Denote the map γ of [CKK+16, Lemma 5.2] for the settings (a) and (b) below by γ+ and γ−,v (for each v∈Tf), respectively.
(a) A=πT, f=ρ∘κT,
f:πT→Gal(F+/F)≅Γ where πT→Gal(F+/F) is the projection.
(b) A=πv, f=ρ∘κv, f:πv→πv/Iv→f′Γ for f′ satisfying φ∘f′=(ρ∘κv)∣πv/Iv∈Hom(πv/Iv,A).
Denote γ+,v:=γ+∘iv,T∈Hom(πv,Z/2Z) and ψv:=γ+,v−γ−,v for each v∈Tf. Note that γ−,v is unramified since it factors through πv/Iv. For v∈X∞, κv=0 so invv(ρv∗(α)∪ψv)=0 for ρv:=ρ∘κv.
where r is the number of primes in Sf which are inert in Fα.
Assumption 4.4**.**
K⊂L* and E are number fields, D>1 is a squarefree integer such that
(1) Gal(L/Q)≅Γ and dL is odd.
(2) Gal(K/Q)≅A and K is totally real.
(3) [E:Q] is odd and E∩L=Q.
(4) D divides dK, Q(D)⊂K and K/Q(D) is unramified at all primes.*
Proposition 4.5**.**
Let t>1 be a squarefree integer prime to D and F=Q(Dt)E satisfies
Q(Dt)∩L=Q.
Then F−=KF and F+=LF satisfy Assumption 4.1.
Proof.
Denote E′=Q(Dt). By the relations E∩L=E′∩L=E∩E′=Q and the fact that E′/Q and L/Q are Galois,
[TABLE]
(the last equality is due to EL∩E′L=L from ([EL:L],[E′L:L])=([E:Q],2)=1) so F∩L=Q.
For each real prime v of F, K/Q is unramified at v so F−/F is also unramified at v. Other conditions can be proved exactly as [CKK+16, Proposition 5.10].
∎
Now suppose that Fα=F(M)⊂F− for some divisor M>0 of D. Denote Q1=Q(M), Q2=Q(N) for N=Dt/M and DL/K:=NmK/Q(ΔL/K)=dL/dK2.
Theorem 4.6**.**
Suppose Assumption 4.4 holds and choose F⊂Fα⊂F−⊂F+ as above, ρ and c as Assumption 4.1. Then,
[TABLE]
where s is the number of prime divisors of (DL/K,D) which are inert either in Q1 or in Q2.
Proof.
We use Theorem 4.3. Following the proof of [CKK+16, Theorem 5.13], we can deduce that
[TABLE]
Let F0=Q(Dt), p∈Sf be a prime above p and p0=p∩F0 be a prime of F0.
Suppose p does not divide D.
If p splits in F0, then pOF=p1⋯pm for some even integer m and pi are all inert or all split in Fα, so they do not change the parity of r of Theorem 4.3.
If p is inert in F0, then p0 splits in F0(M) by [CKK+16, Lemma 5.12] and [F:F0]=[E:Q] is odd so p also splits in Fα. (Note that E∩F0=Q.)
Now suppose that p divides D. Then p is the only prime of F above p. Since [F:F0] is odd, p is inert in Fα if and only if p0 is inert in F0(M). This is equivalent to the fact that p is inert either in Q1 or in Q2.
∎
Remark 4.7**.**
In Proposition 5.10 of [CKK+16], F=Q(−∣D∣⋅t) can be generalized to F=Q(−∣D∣⋅t)E for every number field E of odd degree such that E∩L=Q.
Now we give explicit computations of CSc for A=Z/2Z, A=Z/2Z×Z/2Z and A=S4.
Case I. A=Z/2Z: Let A=Z/2Z, Γ=Z/4Z and p be a prime congruent to 1 modulo 4. Then K=Q(p), the degree 4 subfield L of Q(μp) and D=p satisfy Assumption 4.4. Let F=Q(pt)E for a squarefree integer t>1 prime to p and a number field E of odd degree.
Proposition 4.8**.**
Let Fα=F−=FK, F+=LF and ρ and c be chosen as above. Then,
[TABLE]
Case II. A=Z/2Z×Z/2Z: Let A=Z/2Z×Z/2Z, Γ=Q8 (the quaternion group) and d1,d2>1 be squarefree integers such that d1≡d2≡1(mod4) and (d1,d2)=1.
Suppose that there is a number field L containing Q(d1,d2) such that Gal(L/Q)≅Q8 and dL is odd.
Then K=Q(d1,d2), L and D=d1d2 satisfy Assumption 4.4.
By [CKK+16, Proposition 5.15], a prime p divides (D,DL/K) if and only if p divides D.
Let F=Q(d1d2⋅t)E (t>1 is a squarefree integer prime to d1d2, E is a number field of odd degree) and
[TABLE]
Since Hom(A,Z/2Z) is of order 4, these are all quadratic subfields of FK over F. Suppose that Q(d1d2t)∩L=Q. Then d1d2t∈L so L=Q(d1,d2,d1d2t)=Q(d1,d2,t) and Gal(L/Q)≅(Z/2Z)3, which is a contradiction. Thus Q(d1d2⋅t)∩L=Q.
Proposition 4.9**.**
Let Fαi=Fi, F−=FK, F+=FL and ρ and ci=αi∪ϵ be chosen as above. Then,
[TABLE]
Two examples of L,K for A=Z/2Z×Z/2Z, Γ=Q8 in [CKK+16, p. 21] can be used in our situation. Let
[TABLE]
(LMFDB [LMFDB1]) be the irreducible polynomial over Q and β be a root of g(x). Also let
L=Q(β), K=Q(5,29) and D=5⋅29.
Then K⊂L, Gal(L/Q)≅Q8 and dL=34⋅56⋅296 is odd. Let F=Q(145⋅t)E, where t>1 is a squarefree integer prime to 145 and E is a number field of odd degree.
Corollary 4.10**.**
Let ρ and ci=αi∪ϵ be chosen as above. Then,
[TABLE]
Let
[TABLE]
(LMFDB [LMFDB2]) be the irreducible polynomial over Q and β be a root of g(x). Also let
L=Q(β), K=Q(5,21), D=5⋅21
and F=Q(105⋅t)E, where t>1 is a squarefree integer prime to 105 and E is a number field of odd degree.
Corollary 4.11**.**
Let ρ and ci=αi∪ϵ be chosen as above. Then,
[TABLE]
Now let A=Z/2Z×Z/2Z and Γ=D4, the dihedral group of order 8. Since K is totally imaginary in the example in [CKK+16], we have to find a new example. Let
[TABLE]
(LMFDB [LMFDB3]) which is irreducible over Q and let β be a root of g(x). Also let
L=Q(β), K=Q(5,29) and D=5⋅29.
Then K, L and D satisfy Assumption 4.4 and DL/K=52. Let F=Q(145⋅t)E (t>1 is a squarefree integer prime to 145 and E is a number field of odd degree), F1=F(5), F2=F(29) and F3=F(145). We can check that Q(145⋅t)∩L=Q as before.
Proposition 4.12**.**
Let Fαi=Fi, F−=FK, F+=FL and ρ and ci=αi∪ϵ be chosen as above. Then,
[TABLE]
Case III. A=S4:
Let A=S4, the symmetric group of degree 4. There is a unique surjective map α:A→Z/2Z and three non-trivial central extensions Γi (1≤i≤3) of A by Z/2Z:
Γ1=GL(2,F3), Γ2 is the transitive group ‘16T65’ in [KM] and Γ3=SL(2,Z/4Z).
Let Γ=Γ1 and suppose that Q⊂Q(D)⊂K⊂L and E satisfy Assumption 4.4. Let F=Q(Dt)E, where t>1 is a squarefree integer prime to D.
Since Γ1 has a unique subgroup of order 24 and Q(Dt)=Q(D), Q(Dt)∩L=Q.
Proposition 4.13**.**
Let Fα=F(D), F−=FK, F+=FL and ρ and c=α∪ϵ as above. Then,
[TABLE]
Let
[TABLE]
(LMFDB [LMFDB4], [LMFDB5]) be irreducible polynomials over Q, D=7537 and L and K be the splitting fields of g1(x) and g2(x), respectively. Then Gal(L/Q)≅Γ, Gal(K/Q)≅A and K is totally real.
Also dK=753712 and dL=324⋅753724 (dK and dL can be calculated from the data of [LMFDB4], [LMFDB5] by using the conductor-discriminant formula), so DL/K=324 and DK/Q(D)=1.
Thus Q⊂Q(D)⊂K⊂L and E satisfy Assumption 4.4 for a number field E of odd degree such that E∩L=Q.
Let F=Q(7537⋅t)E, where t>1 is a squarefree integer prime to 7537.
Corollary 4.14**.**
Let Fα=F(7537), F−=FK, F+=FL and ρ and c be chosen as above. Then,
(LMFDB [LMFDB6]) be irreducible polynomials over Q, D=2777 and L and K be the splitting fields of g1(x) and g2(x), respectively. Then by [CKK+16, Lemma 5.22] and the fact that K is totally real, Q⊂Q(D)⊂K⊂L and E satisfy Assumption 4.4 for a number field E of odd degree such that E∩L=Q and Q(2777⋅t)∩L=Q for squarefree t>1 prime to 2777. Let F=Q(2777⋅t)E, where t>1 is a squarefree integer prime to 2777.
Proposition 4.15**.**
Let Fα=F(2777), F−=FK, F+=FL and ρ and c be chosen as above. Then,
[TABLE]
Remark 4.16**.**
Let F=Q(2777⋅7537)E and c1,c2∈H3(S4,Z/2Z) are given by c of Proposition 4.13 and 4.15, respectively. Then,
CSc1([ρ])=0* and (27777537)=−1⇒CSc2([ρ])=21,*
so CSc([ρ]) can be different when both the number field F and the gauge group A are same.
4.2 Biquadratic fields with n=2
In this subsection, we provide an analogue of Theorem 4.6 for the compositum of a biquadratic field and a number field of odd degree. Unfortunately, CSc([ρ]) is always zero in this case.
Assumption 4.17**.**
K⊂L* and E are number fields, D1,D2=1 are squarefree integers such that
(1) Gal(L/Q)≅Γ and dL is odd.
(2) Gal(K/Q)≅A and K is totally real when both D1 and D2 are positive.
(3) [E:Q] is odd and E∩L=Q.
(4) (D1,D2)=1 and D1D2 divides dK.
(5) Q(D1,D2)⊂K and K/Q(D1,D2) is unramified at all primes.*
Let F=Q(D1t1,D2t2)E, where t1,t2>1 are squarefree integers such that D1,D2,t1,t2 are pairwise coprime. Denote F0=Q(D1t1,D2t2) and suppose that F0∩L=Q. Then we can prove F∩L=Q exactly as the proof of Proposotion 4.5.
Proposition 4.18**.**
Let K, L, D1, D2 and E satisfy Assumption 4.17 and F is given as above (with the assumption F0∩L=Q). Then F−=KF and F+=LF satisfy Assumption 4.1.
Now suppose that Fα=F(M)⊂F− for some M=1 dividing D1D2. Denote Q1=Q(M) and Q2=Q(N) for N=D1D2t1t2/M.
Theorem 4.19**.**
Suppose we are in Assumption 4.17 and choose F⊂Fα⊂F−⊂F+ as above, ρ and c as Assumption 4.1. Then,
[TABLE]
Proof.
We can prove that
[TABLE]
by using Abhyankar’s lemma as in the proof of [CKK+16, Theorem 5.13]. By Theorem 4.3, CSc([ρ])≡2r(modZ) where r is the number of primes in Sf which are inert in Fα.
Let p∈Sf be a prime above p and p0=p∩F0. For primes of F above p, they are all inert or all split in Fα. Thus if p splits into two or four primes in F0, these do not change the parity of r, so we do not need to consider them.
Now suppose that p0 is the only prime of F0 above p. If p is unramified in F0/Q, then its inertia degree in F0/Q is 4 so
[TABLE]
a contradiction. Suppose that both the ramification index and the inertia degree of p in F0/Q are 2. One can choose
[TABLE]
which is unramified at p. Since [F:F0]=[E:Q] is odd, Fα/F is inert at p if and only if F0(M)/F0 is inert at p0. In this case, the inertia degree of p in F0(M)/Q is 4 and F0(M)/F1 is ramified at p so the inertia degree of p in F1/Q is also 4, which is also a contradiction.
∎
4.3 Non-vanishing examples with general n and non-abelian gauge group
In this subsection, F is always totally imaginary. In [BCG+18], the following is proved.
Theorem 4.20**.**
([BCG+18, Theorem 1.2]) Let n>1 be an integer and c be a fixed generator of H3(Z/nZ,Z/nZ). Then, there are infinitely many totally imaginary number fields F with a cyclic unramified Kummer extension K/F of degree n such that for the natural map ρ:π↠Gal(K/F)≃Z/nZ,
[TABLE]
For n≥3 and a non-cyclic gauge group A, nothing was known about the non-triviality of CSc. Based on the theorem above, we prove for a large family of finite groups, there are infinitely many totally imaginary number fields F such that CSc([ρ])=0 for some ρ and c.
Lemma 4.21**.**
Let φ:B→A be a homomorphism of finite groups, ρ∈Homcont(π,B) and c∈H3(A,Z/nZ). For ρ′=φ∘ρ:π→A and c′=φ∗(c)∈H3(B,Z/nZ),
[TABLE]
Proof.
(ρ′)∗(c)=(φ∘ρ)∗(c)=ρ∗φ∗(c)=ρ∗(c′).
∎
Let A be a finite group and φ:Z/nZ→A be a group homomorphism. If there exists c∈H3(A,Z/nZ) such that φ∗(c) is a generator of H3(Z/nZ,Z/nZ), then by Theorem 4.20 and Lemma 4.21,
[TABLE]
for infinitely many number fields F with some ρ∈Homcont(π,Z/nZ).
For any finite group G, let
[TABLE]
be the Bockstein homomorphism coming from the exact sequence 0→Z/nZ→nZ/n2Z→Z/nZ→0.
For the identity map Id∈Hom(Z/nZ,Z/nZ)=H1(Z/nZ,Z/nZ), Id∪δ(Id)∈H3(Z/nZ,Z/nZ) is a generator of the group H3(Z/nZ,Z/nZ) ([CKK+19, p. 5684]).
Suppose that there is ψ∈Hom(A,Z/nZ) such that ψ∘φ=Id and denote c=ψ∪δ(ψ)∈H3(A,Z/nZ).
Since the following diagram
[TABLE]
commutes,
[TABLE]
so φ∗(c) is a generator of H3(Z/nZ,Z/nZ).
Theorem 4.22**.**
Let G be a finite group, α:Z/nZ→Aut(G) a group homomorphism and A=G⋊αZ/nZ the semidirect product of G by Z/nZ with respect to α.
Then, there are infinitely many totally imaginary number fields F such that
[TABLE]
for some ρ∈Homcont(π,A) and c∈H3(A,Z/nZ).
Proof.
By Theorem 4.20, there are infinitely many totally imaginary number fields F with with a cyclic unramified Kummer extension K/F of degree n such that for the natural map ρ′:π↠Gal(K/F)≃Z/nZ,
[TABLE]
By the discussion above, it is enough to show that there are group homomorphisms φ:Z/nZ→A and ψ:A→Z/nZ such that ψ∘φ=Id.
Since A is a semidirect product of G by Z/nZ, there are
ψ∈Hom(A,Z/nZ) and φ∈Hom(Z/nZ,A)
such that ψ∘φ=Id.
Then for c=ψ∪δ(ψ)∈H3(A,Z/nZ)
and ρ=φ∘ρ′∈Homcont(π,A), we have (Lemma 4.21)
[TABLE]
Example 4.23**.**
For d≥3, the Heisenberg group
[TABLE]
(with matrix multiplication) can be represented as a semidirect product
[TABLE]
so Theorem 4.22 can be applied to the case A=Hd(Z/nZ).
Example 4.24**.**
Let Fq be the finite field of order q=pk≥3 and r be a positive integer. Then the general linear group GL(r,Fq) can be represented as a semidirect product SL(r,Fq)⋊(Fq)× and (Fq)× is a cyclic group of order q−1, so Theorem 4.22 can be applied to n=q−1 and A=GL(r,Fq).
Example 4.25**.**
Let p be a prime. If p is odd, there are two non-abelian groups of order p3 : H3(Z/pZ) and Z/p2Z⋊Z/pZ. Theorem 4.22 can be applied to both groups. If p=2, then non-abelian groups of order 8 are D4≅Z/4Z⋊Z/2Z and Q8. Since Q8 is not a semidirect product of its proper subgroups, Theorem 4.22 cannot be applied.
Appendix A Completed étale cohomology of number fields
In this section, we review the method of Zink [Zin78] and Conrad-Masullo [CM] of generalizing the étale cohomology of X=Spec(OF) for totally imaginary number fields F, which was studied by Mazur [Maz73], to arbitrary number fields. And we give an alternative viewpoint of the arithmetic Chern-Simons theory by using this generalized étale cohomology. We closely follow the exposition of [CM].
A.1 Completed small étale sites
Let η:Spec(F)→X be a generic point of X and denote its image in X also by η. For a scheme Y and a group G, denote the category of abelian étale sheaves on Y by AbY and the category of G-modules by ModG. For F∈AbX, η∗(F)∈AbSpec(F) and the functor AbSpec(F)→ModGF (G↦⟶limF⊆L⊆F,[L:F]<∞G(Spec(L))) is an equivalence of categories ([Fu11, Proposition 5.7.8]) so η∗(F) corresponds to a GF-module. (Denote by Fη.)
Let X∞={v1,⋯,vr} be the set of all real places of F and X:=X∪X∞. We endow X with the topology whose closed sets are finite subsets of X∖{η}. Denote an open set of X by U and define U∞:=U∩X∞ and U:=U∩X. For an open subset U⊂X, define U:=U∪X∞.
For each real place v of F, let v be a fixed extension of v to F and denote the decomposition group and the inertia group of v by Dv and Iv, respectively.
Since v is a real place, Iv=Dv=Gal(Fv/Fv)≅Z/2Z.
For F∈AbU, Iv acts on Fη∈ModGF via a natural homomorphism Iv→GF.
For x∈X∖{η}, its decomposition group and inertia group are given by Dx:=Gal(Fx/Fx) and Ix:=Gal(Fx/Fxun), where Fxun is the maximal unramified extension of Fx in Fx.
Definition A.1**.**
An abelian sheafF on a non-empty open subset U⊂X is a triple
[TABLE]
where v varies through U∞, Fv are abelian groups, F is an abelian étale sheaf on U and φv:Fv→FηIv are group homomorphisms. We call Fv the stalk of F at v, and we also denote the stalk Fx at any x∈U by Fx. F is called constructible if F is constructible and Fv is finite for each v∈U∞.
Definition A.2**.**
Let \widetilde{\mathcal{F}}=(\big{\{}\widetilde{\mathcal{F}}_{\widetilde{v}}\big{\}},\mathcal{F},\big{\{}\varphi_{\widetilde{v}}\big{\}}) and \widetilde{\mathcal{G}}=(\big{\{}\widetilde{\mathcal{G}}_{\widetilde{v}}\big{\}},\mathcal{G},\big{\{}\psi_{\widetilde{v}}\big{\}}) be abelian sheaves on U. A morphismf:F→G of abelian sheaves on U is a triple f:=((fv),f) such that f:F→G is a morphism of sheaves and
for each v∈U∞,
fv:Fv→Gv is a group homomorphism and fη∘φv=ψv∘fv. The kernel and cokernel of f is defined by \ker(\widetilde{f}):=(\big{\{}\ker(\widetilde{f}_{\widetilde{v}})\big{\}},\ker(f),\big{\{}\varphi^{\prime}_{\widetilde{v}}\big{\}}) and \operatorname{coker}(\widetilde{f}):=(\big{\{}\operatorname{coker}(\widetilde{f}_{\widetilde{v}})\big{\}},\operatorname{coker}(f),\big{\{}\psi^{\prime}_{\widetilde{v}}\big{\}}) for canonical group homomorphisms φv′ and ψv′.
Denote the category of abelian sheaves on U by AbU. To develop a cohomology theory on U, we need to construct an étale site on which the category of abelian sheaves is AbU. For any scheme Y, define Y(R):=Hom(Spec(R),Y).
A morphism of schemes f:Y→Y′ induces a map fR:Y(R)→Y′(R) and X(R) can be identified with X∞.
Let SchX be the category whose objects are pairs Y=(Y,Y∞) for an étale X-scheme Y and a subset Y∞⊂Y(R), and morphisms g:Y→Y′ are morphisms g:Y→Y′ of X-schemes such that gR(Y∞)⊂Y′∞.
Now let EtU be the category whose objects are the morphisms Y→U in SchX and morphisms are defined over U in the evident manner.
A covering in EtU is a family of morphisms \big{\{}\widetilde{f_{i}}:\widetilde{Y_{i}}\rightarrow\widetilde{Y}\big{\}} such that \big{\{}f_{i}:Y_{i}\rightarrow Y\big{\}} is a covering in EtU (so ⋃i∈Ifi(Yi)=Y) and ⋃i∈IfiR(Yi∞)=Y∞.
These coverings define the étale topology on U, so they define the small étale site Ueˊt. Denote the category of abelian sheaves on Ueˊt by AbU.
Proposition A.3**.**
([CM, Theorem 2.4.3]) The categories AbU and AbU are equivalent.
For an abelian group A, let AU be the constant sheaf on Ueˊt defined by A.
From the proof of the above proposition in [CM], AU corresponds to (\big{\{}A\big{\}}_{\widetilde{v}},A_{U},\big{\{}id_{A}\big{\}}_{\widetilde{v}})\in\mathfrak{Ab}_{\widetilde{U}}.
Denote this element also by AU.
We may omit the subscript U of AU when the context is clear.
For F∈AbU,
[TABLE]
where U∞={v1,⋯,vs}, and the fiber product is taken with respect to the natural map F(U)→Fη and the specialization maps Fvk→FηIvkFη.
The right side gives the definition of the global section functor on AbU, namely, Γ(U,⋅):AbU→Ab (F↦F(U)×FηFv1×Fη⋯×FηFvs).
From now on we identify two categories AbU and AbU, and use them without distinction.
A.2 Cohomology theory
Since Γ(U,⋅) is left-exact, its right derived functor Hp(U,F):=RpΓ(U,F) is well-defined for each p≥0.
Let V⊂U be non-empty open subsets of X and S=U∖V.
Then S=Sf∪S∞ for Sf=U∖V and S∞=U∞∖V∞.
Define ΓS(U,F):=ker(F(U)→ker(F(V)) and HSp(U,F):=RpΓS(U,F).
Denote ΓS(U,F) by Γx(U,F) and HSp(U,F) by Hxp(U,F) when S={x}.
Then for F∈AbU, the following local cohomology sequence is exact ([CM, p. 21]).
[TABLE]
Lemma A.4**.**
([CM, Lemma 3.2.3]) For \widetilde{\mathcal{F}}=(\big{\{}\widetilde{\mathcal{F}}_{\widetilde{v}}\big{\}},\mathcal{F},\big{\{}\varphi_{\widetilde{v}}\big{\}})\in\mathbf{Ab}_{\widetilde{U}} and v∈U∞,
[TABLE]
Let U⊂X be a non-empty open subscheme. For each v∈X∞=U∞, denote the algebraic closure of F in its completion Fv≅R by Fvalg. Its positive part, which corresponds to R>0 by the isomorphism Fv≃R is denoted by Fvalg,+. Denote the inclusion of groups Fvalg,+↪Fvalg,× by ιv. From the formula
[TABLE]
Gm,U,ηIv=Fvalg,× and the following definition is well-defined. For the motivation of the definition below, see Example A.8.
Definition A.5**.**
The sheaf Gm,U∈AbU=AbU is defined by the triple
(\big{\{}F_{v}^{alg,+}\big{\}}_{v\in X_{\infty}},\mathbf{G}_{m,U},\big{\{}\iota_{v}\big{\}}_{v\in X_{\infty}}).
Define the sheaf μn,U∈AbU by μn,U:=ker(Gm,U→nGm,U). Since there is an injection Fvalg,+→R>0, ker(Fvalg,+→nFvalg,+)=0 and \mu_{n,\overline{U}}=(\big{\{}0\big{\}}_{v\in X_{\infty}},\mu_{n,U},\big{\{}0\rightarrow\mu_{n}(F_{v}^{alg,+})\big{\}}_{v\in X_{\infty}}). We may omit the subscript U of Gm,U and μn,U when the context is clear.
Even though the cohomology of Gm,U for an arbitrary non-empty open subset U of X is known, we only state the result for the case U=X because this is the only case that we use later. Let OF×,+ be the group of totally positive units of F, and Cl+(F) be the narrow class group of F.
The cohomology of μn,X and Z/nZX will be given in the next subsection. To compute these, we should use Artin-Verdier duality for an arbitrary number field.
A.3 Artin-Verdier duality
Let F∈AbU be a non-empty open subset U of X. For each v∈X∞, Fη is an Iv-module and the norm map Nv on Fη induces a map Nv:H0(Iv,Fη)→H0(Iv,Fη).
Definition A.7**.**
The modified sheaf of F∈AbU is defined by
[TABLE]
Example A.8**.**
(1) Since Gm,U,η=F× and the image of Nv:Gm,U,η→Gm,U,η is Fvalg,+,
[TABLE]
and Nv:H0(Iv,Gm,U,η)→H0(Iv,Gm,U,η) is identified with the inclusion map Fvalg,+Fvalg,×. Thus Gm,U=Gm,U.
(2) Let A be an abelian group. It is easy to show that \widehat{A_{U}}=(\big{\{}A\big{\}},A_{U},\big{\{}A\overset{2}{\rightarrow}A\big{\}})\in\mathbf{Ab}_{\overline{U}}, which is not equal to AU in general. However, there is a natural morphism \widetilde{f}=(\big{\{}A\overset{2}{\rightarrow}A\big{\}},id_{A_{U}}):\widehat{A_{U}}\rightarrow A_{\overline{U}} and it induces an isomorphism Hp(U,AU)→Hp(U,AU) for each p≥1 by the following lemma.
Lemma A.9**.**
Let \widetilde{\mathcal{F}}=(\big{\{}\widetilde{\mathcal{F}}_{\widetilde{v}}\big{\}},\mathcal{F},\big{\{}\varphi_{\widetilde{v}}\big{\}}) and \widetilde{\mathcal{G}}=(\big{\{}\widetilde{\mathcal{G}}_{\widetilde{v}}\big{\}},\mathcal{G},\big{\{}\psi_{\widetilde{v}}\big{\}}) be abelian sheaves on U and f:F→G be a morphism in AbU whose kernel and cokernel are supported at real points. (Equivalently, f:F→G is an isomorphism in AbU.) Then for each p≥1, the map Hp(U,F)→Hp(U,G) induced by f is an isomorphism.
Definition A.10**.**
*Let F∈AbU, j:U→X be an open immersion, X∞={v1,⋯,vr}, p∈Z and HTp denote the p-th Tate cohomology.
(1) The p-th modified étale cohomology groups of F are*
[TABLE]
(2) The p-th compactly supported cohomology groups of F are Hcp(U,F):=Hp(X,j!F).
Example A.11**.**
([CM, Example 5.4.2]) A natural morphism j!Gm,U→Gm,X in AbX induces an isomorphism Hc3(U,Gm,U)=H3(X,j!Gm,U)≃H3(X,Gm,X)≅Q/Z.
Theorem A.12**.**
([CM, Theorem 5.4.4]; Artin-Verdier duality) Let F be a constructible abelian étale sheaf on a dense open subset U of X. The Yoneda pairing
[TABLE]
is a perfect pairing of finite abelian groups for all p∈Z. (ExtUi is defined to be [math] for i<0, so Hcp(U,F)=0 if p>3.)
By Theorem 2.3 and Theorem A.12, two different definitions of compactly supported étale cohomology in Section 2 and Appendix A are naturally identified. For the isomorphism
[TABLE]
and the map
[TABLE]
the arithmetic Chern-Simons action can be expressed as CSc([ρ])=inv(j3(ρ∗(c))).
Acknowledgments
Jungin Lee was supported by a KIAS Individual Grant (SP079601) via the Center for Mathematical Challenges at Korea Institute for Advanced Study.
Jeehoon Park was supported by Samsung Science & Technology Foundation SSTF-BA1502,
the National Research Foundation of Korea (NRF-2021R1A2C1006696) and the National Research Foundation of Korea (NRF) grant funded by the Korea government (MSIT) (No.2020R1A5A1016126).
The second author thanks Hwajong Yoo for providing useful comments on the draft.
Bibliography24
The reference list from the paper itself. Each links out to its DOI / PubMed record.
1[BCG+18] Bleher, F.; Chinburg, T.; Greenberg, R.; Kakde. M.; Pappas, G.; Taylor, M. Cup products in the étale cohomology of number fields, New York J. Math. 24 (2018), 514–542.
2[CKK+16] Chung, H.-J.; Kim, D.; Kim, M.; Park, J.; Yoo, H. Arithmetic Chern-Simons theory II, preprint, ar Xiv:1609.03012 v 3 .
3[CKK+19] Chung, H.-J.; Kim, D.; Kim, M.; Pappas, G.; Park, J.; Yoo, H. Abelian arithmetic Chern-Simons theory and arithmetic linking numbers, Int. Math. Res. Not. (2019), no. 18, 5674–5702.
4[CM] Conrad, B.; Masullo, A. M. Étale cohomology of algebraic number fields, Available at http://pdfs.semanticscholar.org/9a 34/63b 8caeb 15ef 3c 0976789 edb 22e 9d 093e 80e.pdf .
5[DW 90] Dijkgraaf, R.; Witten, E. Topological gauge theories and group cohomology, Comm. Math. Phys. 129 (1990), 393–429.
6[Fu 11] Fu, L. Étale cohomology theory, Nankai Tracts in Mathematics, vol. 13, World Scientific Publishing Company, Singapore, 2011.
7[Kim 15] Kim, M. Arithmetic Chern-Simons theory I, preprint, ar Xiv:1510.05818 v 4 .
8[Kap 96] Kapranov, M. Analogies between number fields and 3-manifolds. Unpublished Note (1996).