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In
number theory Number theory is a branch of pure mathematics devoted primarily to the study of the integers and arithmetic functions. Number theorists study prime numbers as well as the properties of mathematical objects constructed from integers (for example ...
, the class number formula relates many important invariants of an
algebraic number field In mathematics, an algebraic number field (or simply number field) is an extension field K of the field of rational numbers such that the field extension K / \mathbb has finite degree (and hence is an algebraic field extension). Thus K is a ...
to a special value of its Dedekind zeta function.


General statement of the class number formula

We start with the following data: * is a number field. * , where denotes the number of real embeddings of , and is the number of complex embeddings of . * is the Dedekind zeta function of . * is the class number, the number of elements in the
ideal class group In mathematics, the ideal class group (or class group) of an algebraic number field K is the quotient group J_K/P_K where J_K is the group of fractional ideals of the ring of integers of K, and P_K is its subgroup of principal ideals. The ...
of . * is the regulator of . * is the number of roots of unity contained in . * is the discriminant of the extension . Then: :Theorem (Class Number Formula). converges absolutely for and extends to a meromorphic function defined for all complex with only one simple pole at , with residue :: \lim_ (s-1) \zeta_K(s) = \frac This is the most general "class number formula". In particular cases, for example when is a cyclotomic extension of , there are particular and more refined class number formulas.


Proof

The idea of the proof of the class number formula is most easily seen when ''K'' = Q(i). In this case, the ring of integers in ''K'' is the
Gaussian integer In number theory, a Gaussian integer is a complex number whose real and imaginary parts are both integers. The Gaussian integers, with ordinary addition and multiplication of complex numbers, form an integral domain, usually written as \mathbf ...
s. An elementary manipulation shows that the residue of the Dedekind zeta function at ''s'' = 1 is the average of the coefficients of the
Dirichlet series In mathematics, a Dirichlet series is any series of the form \sum_^\infty \frac, where ''s'' is complex, and a_n is a complex sequence. It is a special case of general Dirichlet series. Dirichlet series play a variety of important roles in anal ...
representation of the Dedekind zeta function. The ''n''-th coefficient of the Dirichlet series is essentially the number of representations of ''n'' as a sum of two squares of nonnegative integers. So one can compute the residue of the Dedekind zeta function at ''s'' = 1 by computing the average number of representations. As in the article on the Gauss circle problem, one can compute this by approximating the number of lattice points inside of a quarter circle centered at the origin, concluding that the residue is one quarter of pi. The proof when ''K'' is an arbitrary imaginary quadratic number field is very similar. In the general case, by Dirichlet's unit theorem, the group of units in the ring of integers of ''K'' is infinite. One can nevertheless reduce the computation of the residue to a lattice point counting problem using the classical theory of real and complex embeddings and approximate the number of lattice points in a region by the volume of the region, to complete the proof.


Dirichlet class number formula

Peter Gustav Lejeune Dirichlet Johann Peter Gustav Lejeune Dirichlet (; ; 13 February 1805 – 5 May 1859) was a German mathematician. In number theory, he proved special cases of Fermat's last theorem and created analytic number theory. In analysis, he advanced the theory o ...
published a proof of the class number formula for
quadratic field In algebraic number theory, a quadratic field is an algebraic number field of Degree of a field extension, degree two over \mathbf, the rational numbers. Every such quadratic field is some \mathbf(\sqrt) where d is a (uniquely defined) square-free ...
s in 1839, but it was stated in the language of quadratic forms rather than classes of ideals. It appears that Gauss already knew this formula in 1801. This exposition follows Davenport. Let ''d'' be a fundamental discriminant, and write ''h(d)'' for the number of equivalence classes of quadratic forms with discriminant ''d''. Let \chi = \left(\!\frac\!\right) be the Kronecker symbol. Then \chi is a Dirichlet character. Write L(s,\chi) for the Dirichlet L-series based on \chi. For ''d > 0'', let ''t > 0'', ''u > 0'' be the solution to the Pell equation t^2 - d u^2 = 4 for which ''u'' is smallest, and write :\varepsilon = \frac(t + u \sqrt). (Then \varepsilon is either a fundamental unit of the real quadratic field \mathbb(\sqrt) or the square of a fundamental unit.) For ''d'' < 0, write ''w'' for the number of automorphisms of quadratic forms of discriminant ''d''; that is, :w = \begin 2, & d < -4; \\ 4, & d = -4; \\ 6, & d = -3. \end Then Dirichlet showed that :h(d)= \begin \dfrac L(1,\chi), & d < 0; \\ \dfrac L(1,\chi), & d > 0. \end This is a special case of Theorem 1 above: for a
quadratic field In algebraic number theory, a quadratic field is an algebraic number field of Degree of a field extension, degree two over \mathbf, the rational numbers. Every such quadratic field is some \mathbf(\sqrt) where d is a (uniquely defined) square-free ...
''K'', the Dedekind zeta function is just \zeta_K(s) = \zeta(s) L(s, \chi), and the residue is L(1,\chi). Dirichlet also showed that the ''L''-series can be written in a finite form, which gives a finite form for the class number. Suppose \chi is primitive with prime conductor q. Then : L(1, \chi) = \begin -\dfrac\sum_^ m \left( \dfrac \right), & q \equiv 3 \mod 4; \\ -\dfrac\sum_^ \left( \dfrac \right) \ln\left(\sin \dfrac\right) , & q \equiv 1 \mod 4. \end


Galois extensions of the rationals

If ''K'' is a Galois extension of Q, the theory of
Artin L-function In mathematics, an Artin ''L''-function is a type of Dirichlet series associated to a linear representation ρ of a Galois group ''G''. These functions were introduced in 1923 by Emil Artin, in connection with his research into class field theo ...
s applies to \zeta_K(s). It has one factor of the Riemann zeta function, which has a pole of residue one, and the quotient is regular at ''s'' = 1. This means that the right-hand side of the class number formula can be equated to a left-hand side :Π ''L''(1,ρ)dim ρ with ρ running over the classes of irreducible non-trivial complex linear representations of Gal(''K''/Q) of dimension dim(ρ). That is according to the standard decomposition of the regular representation.


Abelian extensions of the rationals

This is the case of the above, with Gal(''K''/Q) an abelian group, in which all the ρ can be replaced by Dirichlet characters (via class field theory) for some modulus ''f'' called the conductor. Therefore all the ''L''(1) values occur for
Dirichlet L-function In mathematics, a Dirichlet L-series is a function of the form :L(s,\chi) = \sum_^\infty \frac. where \chi is a Dirichlet character and s a complex variable with real part greater than 1 . It is a special case of a Dirichlet series. By anal ...
s, for which there is a classical formula, involving logarithms. By the Kronecker–Weber theorem, all the values required for an analytic class number formula occur already when the cyclotomic fields are considered. In that case there is a further formulation possible, as shown by Kummer. The regulator, a calculation of volume in 'logarithmic space' as divided by the logarithms of the units of the cyclotomic field, can be set against the quantities from the ''L''(1) recognisable as logarithms of cyclotomic units. There result formulae stating that the class number is determined by the index of the cyclotomic units in the whole group of units. In Iwasawa theory, these ideas are further combined with Stickelberger's theorem.


See also

* Brumer–Stark conjecture * Smith–Minkowski–Siegel mass formula


Notes


References

* {{L-functions-footer Algebraic number theory Quadratic forms