Nontrivial Riemann Zeros as Spectrum

Let \Lambda (s) := \Gamma(s+1)\, (1-2^{1-s}) \, \zeta(s) , and denote its set of zeros by \mathcal{Z}_\Lambda := \mathcal{Z}_\zeta \cup \mathcal{Z}_\mathrm{p} , where \mathcal{Z}_\zeta consists of the nontrivial zeros of \zeta(s) and \mathcal{Z}_\mathrm{p} those of the prefactor ( 1-2^{1-s} ) , with s \neq 1 . We introduce a non-symmetric operator \hat{\mathcal{R}} on L^2([0,\infty)) with spectrum

\displaystyle \sigma(\hat{\mathcal{R}}) = \left\{ i\left(1/2- \lambda \right) \mid \lambda \in \mathcal{Z}_\Lambda \right\} \, .

Assuming simplicity of all nontrivial Riemann zeros, we construct the compression \hat{\mathcal{R}}_{\mathcal{Z}_\zeta} of \hat{\mathcal{R}} to the spectral subspace associated with \mathcal{Z}_\zeta, and show that \hat{\mathcal{R}}_{\mathcal{Z}_\zeta} is intertwined with its adjoint by a positive semidefinite operator \hat{W} ; i.e., \hat{W} \, \hat{\mathcal{R}}_{\mathcal{Z}_\zeta} = \hat{\mathcal{R}}_{\mathcal{Z}_\zeta}^\dagger \, \hat{W} with \hat{W} \ge 0 . The positivity of \hat{W} , viewed as an operator-theoretic form of (Bombieri’s refinement of) Weil’s positivity criterion, enforces \Re(\rho)=1/2 for all \rho \in \mathcal{Z}_\zeta , in accordance with the Riemann Hypothesis. Under the same positivity condition, the intertwining relation yields a self-adjoint operator whose spectrum coincides with the set \{ \Im(\rho) \mid \rho \in \mathcal{Z}_\zeta\} . We further extend the framework to accommodate higher-order nontrivial Riemann zeros, should they exist, and to cover any Mellin-transformable L -function satisfying a functional equation.