Let ψn=(−1)n−1\documentclass[12pt]{minimal}
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\begin{document}$\psi_{n}= ( -1 ) ^{n-1}$\end{document}ψ(n)\documentclass[12pt]{minimal}
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\begin{document}$\psi^{ ( n ) }$\end{document} (n=0,1,2,…\documentclass[12pt]{minimal}
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\begin{document}$n=0,1,2,\ldots $\end{document}), where ψ(n)\documentclass[12pt]{minimal}
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\begin{document}$\psi^{ ( n ) }$\end{document} denotes the psi and polygamma functions. We prove that for n≥0\documentclass[12pt]{minimal}
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\begin{document}$n\geq0$\end{document} and two different real numbers a and b, the function x↦ψn−1(∫abψn(x+t)dtb−a)−x\documentclass[12pt]{minimal}
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\begin{document}$$ x\mapsto\psi_{n}^{-1} \biggl( \frac{\int_{a}^{b}\psi_{n}(x+t)\,dt}{b-a} \biggr) -x $$\end{document} is strictly increasing from (−min(a,b),∞)\documentclass[12pt]{minimal}
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\begin{document}$( -\min ( a,b ) ,\infty ) $\end{document} onto (min(a,b),(a+b)/2)\documentclass[12pt]{minimal}
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\begin{document}$( \min ( a,b ) , ( a+b ) /2 ) $\end{document}, which generalizes a well-known result. As an application, the complete monotonicity for a ratio of gamma functions is improved.