60 research outputs found

    Defeating the Kalka--Teicher--Tsaban linear algebra attack on the Algebraic Eraser

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    The Algebraic Eraser (AE) is a public key protocol for sharing information over an insecure channel using commutative and noncommutative groups; a concrete realization is given by Colored Burau Key Agreement Protocol (CBKAP). In this paper, we describe how to choose data in CBKAP to thwart an attack by Kalka--Teicher--Tsaban

    A converse theorem for double Dirichlet series and Shintani zeta functions

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    The main aim of this paper is to obtain a converse theorem for double Dirichlet series and use it to show that the Shintani zeta functions which arise in the theory of prehomogeneous vector spaces are actually linear combinations of Mellin transforms of metaplectic Eisenstein series on GL (2). The converse theorem we prove will apply to a very general family of double Dirichlet series which we now define

    The cubic Pell equation L-function

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    For d>1d > 1 a cubefree rational integer, we define an LL-function (denoted Ld(s)L_d(s)) whose coefficients are derived from the cubic theta function for Q(βˆ’3)\mathbb Q\left(\sqrt{-3}\right). The Dirichlet series defining Ld(s)L_d(s) converges for Re(s)>1\text{Re}(s) > 1, and its coefficients vanish except at values corresponding to integral solutions of mx3βˆ’dny3=1mx^3 - dny^3 = 1 in Q(βˆ’3)\mathbb Q\left(\sqrt{-3}\right), where mm and nn are squarefree. By generalizing the methods used to prove the Takhtajan-Vinogradov trace formula, we obtain the meromorphic continuation of Ld(s)L_d(s) to Re(s)>12\text{Re}(s) > \frac{1}{2} and prove that away from its poles, it satisfies the bound Ld(s)β‰ͺ∣s∣72L_d(s) \ll |s|^{\frac{7}{2}} and has a possible simple pole at s=23s = \frac{2}{3}, possible poles at the zeros of a certain Appell hypergeometric function, with no other poles. We conjecture that the latter case does not occur, so that Ld(s)L_d(s) has no other poles with Re(s)>12\text{Re}(s) > \frac{1}{2} besides the possible simple pole at s=23s = \frac{2}{3}
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