The 1D transverse-field Ising model H = −J∑σᵢᶻσᵢ₊₁ᶻ − h∑σᵢˣ has an exact quantum phase transition at h/J = 1. At the QCP, the correlation length diverges, the gap closes, and the system is described by a (1+1)D conformal field theory with central charge c = 1/2.