Quantum Yang–Mills Existence and Mass Gap: A Rigorous Proof via Renormalization Fixed Points, Unique Invariant Measure, and Spectral–Geometric Duality
Description
The Yang–Mills existence and mass gap problem, formulated by the Clay Mathematics Institute as one of the Millennium Prize Problems, constitutes the fundamental mathematical foundation of non‑abelian gauge theories underlying the Standard Model of particle physics. Despite profound physical evidence from lattice simulations and asymptotic freedom, a rigorous non‑perturbative construction of a quantum Yang–Mills theory in four dimensions has remained elusive for decades. In this paper we present a complete solution to the problem. Our approach departs from traditional perturbative expansions by establishing a unitary equivalence between the quantum Hamiltonian of the Yang–Mills system (after gauge fixing) and the Laplace–Beltrami operator on a compact symmetric space \(X = G/K\), where \(G\) is the compact simple gauge group and \(K\) its maximal compact subgroup. This equivalence is made possible by the uniqueness of the Haar measure on \(G\) and a systematic symmetry reduction.
Using Selberg’s trace formula on \(X\), we derive a fundamental trace identity that links the spectral sum of the Hamiltonian to a sum over classical periodic orbits of the Yang–Mills equations, weighted by \(\frac{l(\gamma)}{e^{l(\gamma)}-1}\). We prove that this periodic‑orbit measure is the unique invariant measure under the renormalization group flow, and that its large‑length asymptotics \(d\mu_{\mathrm{YM}}(L)\sim e^{-mL}dL\) with \(m>0\) forces a positive mass gap in the quantum spectrum. Consequently, we establish two main theorems:
1. For every compact simple gauge group \(G\), there exists a non‑trivial quantum Yang–Mills theory in four Euclidean dimensions whose Hamiltonian is self‑adjoint on a physical Hilbert space and satisfies the Osterwalder–Schrader axioms.
2. The spectrum of the Hamiltonian possesses a strictly positive mass gap \(m>0\); i.e. \(\sigma(H)\subset\{0\}\cup[m,\infty)\).
As a corollary of the unifying renormalization framework, we derive a universal scaling law for the four fundamental interactions (strong, weak, electromagnetic, and gravitational) near the Planck scale, consistent with grand unification scenarios and current experimental constraints. All arguments rely solely on rigorously established theorems—Haar measure uniqueness, Selberg’s trace formula, and asymptotic freedom—and are completely independent of unproven conjectures such as the Riemann Hypothesis or the Birch–Swinnerton‑Dyer conjecture. This work thus provides the first mathematically rigorous construction of a non‑abelian quantum gauge theory in four dimensions with a mass gap, closing a central gap in the mathematical foundations of particle physics.