Conductor (class field theory)

In algebraic number theory, the conductor of a finite abelian extension of local or global fields provides a quantitative measure of the ramification in the extension. The definition of the conductor is related to the Artin map.

Local conductor

Let L/K be a finite abelian extension of non-archimedean local fields. The conductor of L/K, denoted \mathfrak{f}(L/K), is the smallest non-negative integer n such that the higher unit group

:U^{(n)} = 1 + \mathfrak{m}_K^n = \left\{u\in\mathcal{O}^\times: u \equiv 1\, \left(\operatorname{mod} \mathfrak{m}_K^n\right)\right\}

is contained in NL/K(L×), where NL/K is field norm map and \mathfrak{m}_K is the maximal ideal of K.{{harvnb|Serre|1967|loc=§4.2}} Equivalently, n is the smallest integer such that the local Artin map is trivial on U_K^{(n)}. Sometimes, the conductor is defined as \mathfrak{m}_K^n where n is as above.As in {{harvnb|Neukirch|1999|loc=definition V.1.6}}

The conductor of an extension measures the ramification. Qualitatively, the extension is unramified if, and only if, the conductor is zero,{{harvnb|Neukirch|1999|loc=proposition V.1.7}} and it is tamely ramified if, and only if, the conductor is 1.{{harvnb|Milne|2008|loc=I.1.9}} More precisely, the conductor computes the non-triviality of higher ramification groups: if s is the largest integer for which the "lower numbering" higher ramification group Gs is non-trivial, then \mathfrak{f}(L/K) = \eta_{L/K}(s) + 1, where ηL/K is the function that translates from "lower numbering" to "upper numbering" of higher ramification groups.{{harvnb|Serre|1967|loc=§4.2, proposition 1}}

The conductor of L/K is also related to the Artin conductors of characters of the Galois group Gal(L/K). Specifically,{{harvnb|Artin|Tate|2009|loc=corollary to theorem XI.14, p. 100}}

:\mathfrak{m}_K^{\mathfrak{f}(L/K)} = \operatorname{lcm}\limits_\chi \mathfrak{m}_K^{\mathfrak{f}_\chi}

where χ varies over all multiplicative complex characters of Gal(L/K), \mathfrak{f}_\chi is the Artin conductor of χ, and lcm is the least common multiple.

=More general fields=

The conductor can be defined in the same way for L/K a not necessarily abelian finite Galois extension of local fields.As in {{harvnb|Serre|1967|loc=§4.2}} However, it only depends on Lab/K, the maximal abelian extension of K in L, because of the "norm limitation theorem", which states that, in this situation,{{harvnb|Serre|1967|loc=§2.5, proposition 4}}{{harvnb|Milne|2008|loc=theorem III.3.5}}

: N_{L/K}\left(L^\times\right) = N_{L^{\text{ab}}/K} \left(\left(L^{\text{ab}}\right)^\times \right).

Additionally, the conductor can be defined when L and K are allowed to be slightly more general than local, namely if they are complete valued fields with quasi-finite residue field.As in {{harvnb|Artin|Tate|2009|loc=§XI.4}}. This is the situation in which the formalism of local class field theory works.

=Archimedean fields=

Mostly for the sake of global conductors, the conductor of the trivial extension R/R is defined to be 0, and the conductor of the extension C/R is defined to be 1.{{harvnb|Cohen|2000|loc=definition 3.4.1}}

Global conductor

=Algebraic number fields=

The conductor of an abelian extension L/K of number fields can be defined, similarly to the local case, using the Artin map. Specifically, let θ : Im → Gal(L/K) be the global Artin map where the modulus m is a defining modulus for L/K; we say that Artin reciprocity holds for m if θ factors through the ray class group modulo m. We define the conductor of L/K, denoted \mathfrak{f}(L/K), to be the highest common factor of all moduli for which reciprocity holds; in fact reciprocity holds for \mathfrak{f}(L/K), so it is the smallest such modulus.{{harvnb|Milne|2008|loc=remark V.3.8}}{{harvnb|Janusz|1973|pp=158,168–169}}Some authors omit infinite places from the conductor, e.g. {{harvnb|Neukirch|1999|loc=§VI.6}}

==Example==

  • Taking as base the field of rational numbers, the Kronecker–Weber theorem states that an algebraic number field K is abelian over Q if and only if it is a subfield of a cyclotomic field \mathbf{Q}\left(\zeta_n\right), where \zeta_n denotes a primitive nth root of unity.{{cite book | first1=Yu. I. | last1=Manin | authorlink1=Yuri I. Manin | first2=A. A. | last2=Panchishkin | title=Introduction to Modern Number Theory | series=Encyclopaedia of Mathematical Sciences | volume=49 | edition=Second | year=2007 | isbn=978-3-540-20364-3 | issn=0938-0396 | zbl=1079.11002 | pages=155, 168 }} If n is the smallest integer for which this holds, the conductor of K is then n if K is fixed by complex conjugation and n \infty otherwise.
  • Let L/K be \mathbf{Q}\left(\sqrt{d}\right)/\mathbf{Q} where d is a squarefree integer. Then,{{harvnb|Milne|2008|loc=example V.3.11}}
  • : \mathfrak{f}\left(\mathbf{Q}\left(\sqrt{d}\right)/\mathbf{Q}\right) = \begin{cases}

\left|\Delta_{\mathbf{Q}\left(\sqrt{d}\right)}\right| & \text{for }d > 0 \\

\infty\left|\Delta_{\mathbf{Q}\left(\sqrt{d}\right)}\right| & \text{for }d < 0

\end{cases}

: where \Delta_{\mathbf{Q}(\sqrt{d})} is the discriminant of \mathbf{Q}\left(\sqrt{d}\right)/\mathbf{Q}.

==Relation to local conductors and ramification==

The global conductor is the product of local conductors:For the finite part {{harvnb|Neukirch|1999|loc=proposition VI.6.5}}, and for the infinite part {{harvnb|Cohen|2000|loc=definition 3.4.1}}

:\mathfrak{f}(L/K) = \prod_\mathfrak{p}\mathfrak{p}^{\mathfrak{f}\left(L_\mathfrak{p}/K_\mathfrak{p}\right)}.

As a consequence, a finite prime is ramified in L/K if, and only if, it divides \mathfrak{f}(L/K).{{harvnb|Neukirch|1999|loc=corollary VI.6.6}} An infinite prime v occurs in the conductor if, and only if, v is real and becomes complex in L.

Notes

{{reflist|2}}

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Category:Class field theory