45 research outputs found

    Computing discrete logarithms in subfields of residue class rings

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    Recent breakthrough methods \cite{gggz,joux,bgjt} on computing discrete logarithms in small characteristic finite fields share an interesting feature in common with the earlier medium prime function field sieve method \cite{jl}. To solve discrete logarithms in a finite extension of a finite field \F, a polynomial h(x) \in \F[x] of a special form is constructed with an irreducible factor g(x) \in \F[x] of the desired degree. The special form of h(x)h(x) is then exploited in generating multiplicative relations that hold in the residue class ring \F[x]/h(x)\F[x] hence also in the target residue class field \F[x]/g(x)\F[x]. An interesting question in this context and addressed in this paper is: when and how does a set of relations on the residue class ring determine the discrete logarithms in the finite fields contained in it? We give necessary and sufficient conditions for a set of relations on the residue class ring to determine discrete logarithms in the finite fields contained in it. We also present efficient algorithms to derive discrete logarithms from the relations when the conditions are met. The derived necessary conditions allow us to clearly identify structural obstructions intrinsic to the special polynomial h(x)h(x) in each of the aforementioned methods, and propose modifications to the selection of h(x)h(x) so as to avoid obstructions.Comment: arXiv admin note: substantial text overlap with arXiv:1312.167

    Hybrid moments of the Riemann zeta-function

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    The "hybrid" moments ∫T2T∣ζ(1/2+it)∣k(∫t−Gt+G∣ζ(1/2+ix)∣ℓdx)mdt \int_T^{2T}|\zeta(1/2+it)|^k{(\int_{t-G}^{t+G}|\zeta(1/2+ix)|^\ell dx)}^m dt of the Riemann zeta-function ζ(s)\zeta(s) on the critical line ℜs=1/2\Re s = 1/2 are studied. The expected upper bound for the above expression is Oϵ(T1+ϵGm)O_\epsilon(T^{1+\epsilon}G^m). This is shown to be true for certain specific values of the natural numbers k,ℓ,mk,\ell,m, and the explicitly determined range of G=G(T;k,ℓ,m)G = G(T;k,\ell,m). The application to a mean square bound for the Mellin transform function of ∣ζ(1/2+ix)∣4|\zeta(1/2+ix)|^4 is given.Comment: 27 page
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