<p>For a number field <i>K</i>, the associated Dedekind zeta function <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\zeta _K(s)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>ζ</mi> <mi>K</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>s</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> has a simple pole at <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(s=1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>s</mi> <mo>=</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>, and we denote its residue by <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(R_K\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>R</mi> <mi>K</mi> </msub> </math></EquationSource> </InlineEquation>. Ihara introduced the Euler–Kronecker constant <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\gamma _K\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>γ</mi> <mi>K</mi> </msub> </math></EquationSource> </InlineEquation>. Let <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\ell \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ℓ</mi> </math></EquationSource> </InlineEquation> be an odd prime. We establish lower and upper bounds for <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(R_K\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>R</mi> <mi>K</mi> </msub> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\gamma _K\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>γ</mi> <mi>K</mi> </msub> </math></EquationSource> </InlineEquation> when <i>K</i> is a cyclic extension of degree <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\ell \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ℓ</mi> </math></EquationSource> </InlineEquation> over <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\mathbb {Q}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">Q</mi> </math></EquationSource> </InlineEquation>. These bounds are stronger than those known under the Generalized Riemann Hypothesis (GRH) and are shown to be sharp. However, the trade-off is that they hold only almost surely. Finally, we compute the average of the Euler–Kronecker constants for cyclic fields <i>K</i> of degree <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\ell \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ℓ</mi> </math></EquationSource> </InlineEquation>.</p>

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On the residues and Euler–Kronecker constants of cyclic number fields

  • Peter J. Cho,
  • Gyeongseok Kim

摘要

For a number field K, the associated Dedekind zeta function \(\zeta _K(s)\) ζ K ( s ) has a simple pole at \(s=1\) s = 1 , and we denote its residue by \(R_K\) R K . Ihara introduced the Euler–Kronecker constant \(\gamma _K\) γ K . Let \(\ell \) be an odd prime. We establish lower and upper bounds for \(R_K\) R K and \(\gamma _K\) γ K when K is a cyclic extension of degree \(\ell \) over \(\mathbb {Q}\) Q . These bounds are stronger than those known under the Generalized Riemann Hypothesis (GRH) and are shown to be sharp. However, the trade-off is that they hold only almost surely. Finally, we compute the average of the Euler–Kronecker constants for cyclic fields K of degree \(\ell \) .