Hasse–Davenport Relation

The Hasse–Davenport relations, introduced by , are two related identities for Gauss sums, one called the Hasse–Davenport lifting relation, and the other called the Hasse–Davenport product relation. The Hasse–Davenport lifting relation is an equality in number theory relating Gauss sums over different fields. used it to calculate the zeta function of a Fermat hypersurface over a finite field, which motivated the Weil conjectures.

Gauss sums are analogues of the gamma function over finite fields, and the Hasse–Davenport product relation is the analogue of Gauss's multiplication formula
:$\Gamma(z) \; \Gamma\left(z + \frac\right) \; \Gamma\left(z + \frac\right) \cdots \Gamma\left(z + \frac\right) = (2 \pi)^ \; k^ \; \Gamma(kz). \,\!$
In fact the Hasse–Davenport product relation follows from the analogous multiplication formula for ''p''-adic gamma functions together with the Gross–Koblitz formula of .

Hasse–Davenport lifting relation

Let ''F'' be a finite field with ''q'' elements, and ''F''_s be the field such that 'F''_s:''F''= ''s'', that is, ''s'' is the dimension of the vector space ''F''_s over ''F''.

Let $\alpha$ be an element of $F_s$.

Let $\chi$ be a multiplicative character from ''F'' to the complex numbers.

Let $N_(\alpha)$ be the norm from $F_s$ to $F$ defined by
:$N_(\alpha):=\alpha\cdot\alpha^q\cdots\alpha^.\,$

Let
$\chi'$ be the multiplicative character on $F_s$ which is the composition of $\chi$ with the norm from ''F''_s to ''F'', that is
:$\chi'(\alpha):=\chi(N_(\alpha))$

Let ψ be some nontrivial additive character of ''F'', and let
$\psi'$ be the additive character on $F_s$ which is the composition of $\psi$ with the trace from ''F''_s to ''F'', that is
:$\psi'(\alpha):=\psi(Tr_(\alpha))$

Let
:$\tau(\chi,\psi)=\sum_\chi(x)\psi(x)$
be the Gauss sum over ''F'', and let
$\tau(\chi',\psi')$ be the Gauss sum over $F_s$.

Then the Hasse–Davenport lifting relation states that
:$(-1)^s\cdot \tau(\chi,\psi)^s=-\tau(\chi',\psi').$

Hasse–Davenport product relation

The Hasse–Davenport product relation states that
:$\prod_ \tau(\chi\rho^a,\psi) = -\chi^(m)\tau(\chi^m,\psi)\prod_ \tau(\rho^a,\psi)$
where ρ is a multiplicative character of exact order ''m'' dividing ''q''–1 and χ is any multiplicative character and ψ is a non-trivial additive character.

References

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* Reprinted in Oeuvres Scientifiques/Collected Papers by André Weil

{{DEFAULTSORT:Hasse-Davenport Relation
Cyclotomic fields