Integral Representations of Riemann auxiliary function
Abstract
We prove that the auxiliary function R(s) has the integral representation \[ R(s)=-2s πseπ i s/4(s)∫0∞ ys1-e-π y2+π ω y1-e2π ω y\,dyy, ω=eπ i/4, s>0,\] valid for σ>0. The function in the integrand 1-e-π y2+π ω y1-e2π ω y is entire. Therefore, no residue is added when we move the path of integration.
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