Lehmer pairs and binomial series

Kapitonets Kirill

Published: 2025/8/31

Abstract

The paper defines a generalized Hardy function and simulates the zero of the Zeta function that does not lie on a critical line. $$Z_\alpha=\Re\zeta(\alpha+it)e^{i\theta(t)}$$ where \par $$e^{i\theta(t)}=\pi^{-it/2}\frac{\Gamma(1/4+it/2)}{|\Gamma(1/4+it/2)|}$$ \par Using the binomial series and the generalized summation method, the formula for the generalized Hardy function is obtained. $$Z_\alpha =Z_0+\sum^{\infty}_{k=1}(-1)^k\frac{\alpha(\alpha-1)(\alpha-2)...(\alpha-k+1)}{k!}Q_k$$ \par where \par $Z_\alpha$ is a generalized Hardy function on a line $\alpha+it$; \par $Z_0$ is a generalized Hardy function on a line $it$; $$Q_k=\sum^\infty_{n=2}\Big(\frac{n-1}{n}\Big)^kT_n;$$ $$T_n=\cos((\theta(t)-t\log(n))\delta^{(k)}_{m,n};$$ $$\delta^{(k)}_{m,n}=\frac{\sum^m_{n-1}C^{k-1}_{m-k-n}}{ C^k_{m+k}};$$ $\delta^{(k)}_{m,n}$ is the coefficient obtained using Cesaro's generalized summation method of k order. \par Based on the obtained formula, Gram points of the third kind are determined, the formation condition is considered, and a new definition of Lehmer pairs is given. \par The main result of the work is that we obtain a sequence of functions that tends to the Hardy function, and the zeros tend to the zeros of the Hardy function. \par $$Z_{\alpha,0}=Z_0$$ $$Z_{\alpha,k}=Z_{\alpha,k-1}-P_k$$ where $$P_k=(-1)^{k-1}\frac{\alpha(\alpha-1)(\alpha-2)...(\alpha-k+1)}{k!}Q_k$$ \par Based on the analysis of the obtained sequence of functions, it is shown that the distance between pairs of Lehmer can be arbitrarily small, while always remaining greater than zero. \par Thus, all Lehmer pairs of the Hardy function are real zeros, and the assumption formulated in 1956 that the Hardy function can have a negative maximum or a positive minimum turned out to be false.