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The 1D Ising model is exactly solvable via the transfer matrix T:
T = [[e^(J+h), e^(−J)], [e^(−J), e^(J−h)]]
Z = Tr(Tᴺ) = λ₊ᴺ + λ₋ᴺ. Correlation length ξ = −1/ln(λ₋/λ₊). In 1D, no phase transition for T>0 — spins are disordered. The correlation length diverges only at T→0.