The Hasse–Davenport relations, introduced by Davenport and Hasse (1935), 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. Weil (1949) 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
Γ ( z ) Γ ( z + 1 k ) Γ ( z + 2 k ) ⋯ Γ ( z + k − 1 k ) = ( 2 π ) k − 1 2 k 1 / 2 − k z Γ ( k z ) . {\displaystyle \Gamma (z)\;\Gamma \left(z+{\frac {1}{k}}\right)\;\Gamma \left(z+{\frac {2}{k}}\right)\cdots \Gamma \left(z+{\frac {k-1}{k}}\right)=(2\pi )^{\frac {k-1}{2}}\;k^{1/2-kz}\;\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 Gross & Koblitz (1979).
Hasse–Davenport lifting relation Let F be a finite field with q elements, and Fs be the field such that [Fs:F] = s, that is, s is the dimension of the vector space Fs over F. Let α {\displaystyle \alpha } be an element of F s {\displaystyle F_{s}} . Let χ {\displaystyle \chi } be a multiplicative character from F to the complex numbers. Let N F s / F ( α ) {\displaystyle N_{F_{s}/F}(\alpha )} be the norm from F s {\displaystyle F_{s}} to F {\displaystyle F} defined by
N F s / F ( α ) := α ⋅ α q ⋯ α q s − 1 . {\displaystyle N_{F_{s}/F}(\alpha ):=\alpha \cdot \alpha ^{q}\cdots \alpha ^{q^{s-1}}.\,}
Let
χ ′ {\displaystyle \chi '} be the multiplicative character on F s {\displaystyle F_{s}} which is the composition of χ {\displaystyle \chi } with the norm from Fs to F, that is
χ ′ ( α ) := χ ( N F s / F ( α ) ) {\displaystyle \chi '(\alpha ):=\chi (N_{F_{s}/F}(\alpha ))}
Let ψ be some nontrivial additive character of F, and let
ψ ′ {\displaystyle \psi '} be the additive character on F s {\displaystyle F_{s}} which is the composition of ψ {\displaystyle \psi } with the trace from Fs to F, that is
ψ ′ ( α ) := ψ ( T r F s / F ( α ) ) {\displaystyle \psi '(\alpha ):=\psi (Tr_{F_{s}/F}(\alpha ))}
Let
τ ( χ , ψ ) = ∑ x ∈ F χ ( x ) ψ ( x ) {\displaystyle \tau (\chi ,\psi )=\sum _{x\in F}\chi (x)\psi (x)}
be the Gauss sum over F, and let
τ ( χ ′ , ψ ′ ) {\displaystyle \tau (\chi ',\psi ')} be the Gauss sum over F s {\displaystyle F_{s}} . Then the Hasse–Davenport lifting relation states that
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