<p>For any <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(a\in {\mathbb {C}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mo>∈</mo> <mi mathvariant="double-struck">C</mi> </mrow> </math></EquationSource> </InlineEquation>, the zeros of <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\zeta (s)-a\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ζ</mi> <mo stretchy="false">(</mo> <mi>s</mi> <mo stretchy="false">)</mo> <mo>-</mo> <mi>a</mi> </mrow> </math></EquationSource> </InlineEquation>, denoted by <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\rho _a=\beta _a+\textrm{i}\gamma _a\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>ρ</mi> <mi>a</mi> </msub> <mo>=</mo> <msub> <mi>β</mi> <mi>a</mi> </msub> <mo>+</mo> <mtext>i</mtext> <msub> <mi>γ</mi> <mi>a</mi> </msub> </mrow> </math></EquationSource> </InlineEquation>, are called the <i>a</i>-points of the Riemann zeta function <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\zeta (s)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ζ</mi> <mo stretchy="false">(</mo> <mi>s</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>. In this paper, we reformulate some basic results about the <i>a</i>-points of <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\zeta (s)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ζ</mi> <mo stretchy="false">(</mo> <mi>s</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> shown by Garunkštis and Steuding. We then deduce an asymptotic expansion of the sum <Equation ID="Equ31"> <EquationSource Format="TEX">\(\begin{aligned} S_T(a,\delta )=\sum _{\tau &lt;\gamma _a\leqslant T}\zeta '(\rho _a+\textrm{i}\delta )X^{\rho _a},\quad T\rightarrow \infty , \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <msub> <mi>S</mi> <mi>T</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>a</mi> <mo>,</mo> <mi>δ</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <munder> <mo>∑</mo> <mrow> <mi>τ</mi> <mo>&lt;</mo> <msub> <mi>γ</mi> <mi>a</mi> </msub> <mo>⩽</mo> <mi>T</mi> </mrow> </munder> <msup> <mi>ζ</mi> <mo>′</mo> </msup> <mrow> <mo stretchy="false">(</mo> <msub> <mi>ρ</mi> <mi>a</mi> </msub> <mo>+</mo> <mtext>i</mtext> <mi>δ</mi> <mo stretchy="false">)</mo> </mrow> <msup> <mi>X</mi> <msub> <mi>ρ</mi> <mi>a</mi> </msub> </msup> <mo>,</mo> <mspace width="1em" /> <mi>T</mi> <mo stretchy="false">→</mo> <mi>∞</mi> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(X&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>X</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\tau \geqslant |\delta |+1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>τ</mi> <mo>⩾</mo> <mo stretchy="false">|</mo> <mi>δ</mi> <mo stretchy="false">|</mo> <mo>+</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> are fixed, and <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(0\ne \delta =\frac{2\pi \alpha }{\log \frac{T}{2\pi X}}\ll 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>≠</mo> <mi>δ</mi> <mo>=</mo> <mfrac> <mrow> <mn>2</mn> <mi>π</mi> <mi>α</mi> </mrow> <mrow> <mo>log</mo> <mfrac> <mi>T</mi> <mrow> <mn>2</mn> <mi>π</mi> <mi>X</mi> </mrow> </mfrac> </mrow> </mfrac> <mo>≪</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>. We also find the interesting varied behavior of <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(S_T(a,\delta )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>S</mi> <mi>T</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>a</mi> <mo>,</mo> <mi>δ</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> in different <i>X</i> ranges, which is more complicated than those described previously by Gonek and Pearce-Crump.</p>

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Note on the a -points of the Riemann zeta function

  • Peng-Cheng Hang,
  • Liangjian Hu,
  • Min-Jie Luo

摘要

For any \(a\in {\mathbb {C}}\) a C , the zeros of \(\zeta (s)-a\) ζ ( s ) - a , denoted by \(\rho _a=\beta _a+\textrm{i}\gamma _a\) ρ a = β a + i γ a , are called the a-points of the Riemann zeta function \(\zeta (s)\) ζ ( s ) . In this paper, we reformulate some basic results about the a-points of \(\zeta (s)\) ζ ( s ) shown by Garunkštis and Steuding. We then deduce an asymptotic expansion of the sum \(\begin{aligned} S_T(a,\delta )=\sum _{\tau <\gamma _a\leqslant T}\zeta '(\rho _a+\textrm{i}\delta )X^{\rho _a},\quad T\rightarrow \infty , \end{aligned}\) S T ( a , δ ) = τ < γ a T ζ ( ρ a + i δ ) X ρ a , T , where \(X>0\) X > 0 and \(\tau \geqslant |\delta |+1\) τ | δ | + 1 are fixed, and \(0\ne \delta =\frac{2\pi \alpha }{\log \frac{T}{2\pi X}}\ll 1\) 0 δ = 2 π α log T 2 π X 1 . We also find the interesting varied behavior of \(S_T(a,\delta )\) S T ( a , δ ) in different X ranges, which is more complicated than those described previously by Gonek and Pearce-Crump.