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Construction of the two-dimensional O(3) nonlinear sigma model as an interacting continuum quantum field theory with a mass gap

Theorem 1.2: along bare couplings βN=H+log⁡L2πN+O(log⁡N)\beta_N=H+\frac{\log L}{2\pi}N+O(\log N) with spacing L−NL^{-N}, suitably normalized smeared lattice spins converge in law and in all moments; the limiting Schwinger distributions are Euclidean and O(3)O(3) invariant, reflection positive and clustering with factorial bounds, reconstruct a local relativistic theory in 1+11+1 dimensions with a unique vacuum and a Hamiltonian gap m>0m>0 on the whole vacuum complement, and have a nonzero connected four-point function, so the theory is not Gaussian. Theorem 1.1: normalized by susceptibility and second-moment length, the limit exists along every real β→∞\beta\to\infty without subsequences. The companion proves an isolated one-particle mass atom in the spin two-point spectral measure. Not shown: the value of the mass, the S-matrix of the constructed theory, or a continuum construction for other O(N)O(N).

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Prior state unknown→proved

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Occurred: Oct 4, 2026

Delta type: SOURCE CLAIM

Assumptions: VibeMathed verification: unreviewed. Publication: announcement. AI contribution: ai-discovered. VibeMathed editorial classifications, scores, notes, relations, and dataset structure are CC BY 4.0. Source statements and linked content retain their own rights.

Canonical aliases: Construction of the two-dimensional O(3) nonlinear sigma model as an interacting continuum quantum field theory with a mass gap · O(3) sigma model continuum limit with mass gap

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Construction of the two-dimensional O(3) nonlinear sigma model as an interacting continuum quantum field theory with a mass gap parent of this event

VibeMathed record: Construction of the two-dimensional O(3) nonlinear sigma model as an interacting continuum quantum field theory with a mass gap evidence for this event

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Theorem 1.2: along bare couplings βN=H+log⁡L2πN+O(log⁡N)\beta_N=H+\frac{\log L}{2\pi}N+O(\log N) with spacing L−NL^{-N}, suitably normalized smeared lattice spins converge in law and in all moments; the limiting Schwinger distributions are Euclidean and O(3)O(3) invariant, reflection positive and clustering with factorial bounds, reconstruct a local relativistic theory in 1+11+1 dimensions with a unique vacuum and a Hamiltonian gap m>0m>0 on the whole vacuum complement, and have a nonzero connected four-point function, so the theory is not Gaussian. Theorem 1.1: normalized by susceptibility and second-moment length, the limit exists along every real β→∞\beta\to\infty without subsequences. The companion proves an isolated one-particle mass atom in the spin two-point spectral measure. Not shown: the value of the mass, the S-matrix of the constructed theory, or a continuum construction for other O(N)O(N). parent of this event

Input: Sharp mass bounds for the two-dimensional O(4) model evidence for this event

Construction of the two-dimensional O(3) nonlinear sigma model as an interacting continuum quantum field theory with a mass gap evidence for this event

Companion: An Isolated Particle Pole for the Two-Dimensional O(3) Spin Field evidence for this event

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