<p>Let <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\mathcal {S}\)</EquationSource> </InlineEquation> denote the class of univalent functions in the unit disk <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\mathbb {D}:=\{z\in \mathbb {C}:|z|&lt;1\}\)</EquationSource> </InlineEquation> with the form <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(f(z)=z+\sum _{n=2}^{\infty }a_{n}z^{n}\)</EquationSource> </InlineEquation>. The logarithmic inverse coefficients <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\Gamma _{n}\)</EquationSource> </InlineEquation> of <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(f\in \mathcal {S}\)</EquationSource> </InlineEquation> are defined by <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(F_{f^{-1}}(w):=\log \left( f^{-1}(w)/w\right) =2\sum _{n=1}^{\infty }\Gamma _{n}w^{n}\)</EquationSource> </InlineEquation> valid for some disk <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(|w|\le r_{0}(f)\)</EquationSource> </InlineEquation>. The second Hankel determinant of logarithmic inverse coefficients is defined by <Equation ID="Equ27"> <EquationSource Format="TEX">\(\begin{aligned} H_{2}\left( 2\right) \left( F_{f^{-1}}/2\right) =\Gamma _{2}\Gamma _{4}-\Gamma _{3}^{2}. \end{aligned}\)</EquationSource> </Equation>In this paper, we obtain sharp upper bound of the second Hankel determinant <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(H_{2}\left( 2\right) \left( F_{f^{-1}}/2\right) \)</EquationSource> </InlineEquation> of the logarithmic inverse coefficients of starlike and bounded turning functions.</p>

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Sharp Bounds on Second Hankel Determinant for Coefficients of Logarithmic Inverse of Univalent Functions

  • Mohsan Raza

摘要

Let \(\mathcal {S}\) denote the class of univalent functions in the unit disk \(\mathbb {D}:=\{z\in \mathbb {C}:|z|<1\}\) with the form \(f(z)=z+\sum _{n=2}^{\infty }a_{n}z^{n}\) . The logarithmic inverse coefficients \(\Gamma _{n}\) of \(f\in \mathcal {S}\) are defined by \(F_{f^{-1}}(w):=\log \left( f^{-1}(w)/w\right) =2\sum _{n=1}^{\infty }\Gamma _{n}w^{n}\) valid for some disk \(|w|\le r_{0}(f)\) . The second Hankel determinant of logarithmic inverse coefficients is defined by \(\begin{aligned} H_{2}\left( 2\right) \left( F_{f^{-1}}/2\right) =\Gamma _{2}\Gamma _{4}-\Gamma _{3}^{2}. \end{aligned}\) In this paper, we obtain sharp upper bound of the second Hankel determinant \(H_{2}\left( 2\right) \left( F_{f^{-1}}/2\right) \) of the logarithmic inverse coefficients of starlike and bounded turning functions.