2017
DOI: 10.1007/s40993-017-0079-5
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Artin L-functions of small conductor

Abstract: We study the problem of finding the Artin L-functions with the smallest conductor for a given Galois type. We adapt standard analytic techniques to our novel situation of fixed Galois type and obtain much improved lower bounds on the smallest conductor. For small Galois types we use complete tables of number fields to determine the actual smallest conductor.

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Cited by 4 publications
(3 citation statements)
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References 29 publications
(57 reference statements)
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“…This partially explains why our result for Γ(N) is within a factor of 4 of that for normalΓ1false(Nfalse), despite the conductors being much larger. By the Langlands–Tunnell theorem, the Artin conjecture is true for tetrahedral and octahedral representations, so the conclusion of Theorem 1.2 holds unconditionally for those types. In the icosahedral case, by [3] it is enough to assume the Artin conjecture for all representations in a given Galois conjugacy class; that is, if there is a twist‐minimal, even icosahedral representation of conductor 2862 that does not appear in Table 1, then Artin's conjecture is false for at least one of its Galois conjugates.The entries of Table 1 were computed by Jones and Roberts [20] by a thorough search of number fields with prescribed ramification behavior, and we verified the completeness of the list via the trace formula. In principle, the number field search by Jones and Roberts [19] is exhaustive, so it should be possible to prove Theorem 1.2 unconditionally with a further computation, but that has not yet been carried out to our knowledge.For comparison, we note that Buzzard and Lauder [7] have characterized the odd 2‐dimensional representations of conductor 1500 by computing bases of the associated spaces of weight 1 holomorphic modular forms. Theorem 1.1 for normalΓ1false(Nfalse) improves on the result from [6] by extending to nonsquarefree N and increasing the upper bound from 854 to 880.…”
Section: Introductionmentioning
confidence: 97%
See 1 more Smart Citation
“…This partially explains why our result for Γ(N) is within a factor of 4 of that for normalΓ1false(Nfalse), despite the conductors being much larger. By the Langlands–Tunnell theorem, the Artin conjecture is true for tetrahedral and octahedral representations, so the conclusion of Theorem 1.2 holds unconditionally for those types. In the icosahedral case, by [3] it is enough to assume the Artin conjecture for all representations in a given Galois conjugacy class; that is, if there is a twist‐minimal, even icosahedral representation of conductor 2862 that does not appear in Table 1, then Artin's conjecture is false for at least one of its Galois conjugates.The entries of Table 1 were computed by Jones and Roberts [20] by a thorough search of number fields with prescribed ramification behavior, and we verified the completeness of the list via the trace formula. In principle, the number field search by Jones and Roberts [19] is exhaustive, so it should be possible to prove Theorem 1.2 unconditionally with a further computation, but that has not yet been carried out to our knowledge.For comparison, we note that Buzzard and Lauder [7] have characterized the odd 2‐dimensional representations of conductor 1500 by computing bases of the associated spaces of weight 1 holomorphic modular forms. Theorem 1.1 for normalΓ1false(Nfalse) improves on the result from [6] by extending to nonsquarefree N and increasing the upper bound from 854 to 880.…”
Section: Introductionmentioning
confidence: 97%
“…The entries of Table 1 were computed by Jones and Roberts [20] by a thorough search of number fields with prescribed ramification behavior, and we verified the completeness of the list via the trace formula. In principle, the number field search by Jones and Roberts [19] is exhaustive, so it should be possible to prove Theorem 1.2 unconditionally with a further computation, but that has not yet been carried out to our knowledge.…”
Section: Introductionmentioning
confidence: 97%
“…This same general method has been applied in many contexts. For example, simply taking (λ 1 , λ 2 ) = (0, 0) one is saying that certain L-functions coming from number fields can only exist if conductors are large enough [13]. The method, and the more powerful exclusionary techniques of [6], can be extended to establish L-point-free regions of other landscapes.…”
Section: 2mentioning
confidence: 99%