**How many independent local observers are required to uniquely identify one of \ (n = Lᵈ \) independent critical configurations? ** We establish a conditional birthday-style upper bound \ (K^* 2d ₂ L / Hₑ₂ () + O (1) \) assuming spatial decorrelation, with a conjectured factor-2 lower bound. For \ (Sq \) -symmetric Potts models at continuous critical points we conjecture greedy tightness \ (\0, 1\ \). Using sampling data for \ (q=2, 3, 4 \) Potts and the BEG tricritical model, we verify the formula across four universality classes. For Ising (\ (q=2 \) ), a Temperley-Lieb algebra decomposition gives an exact orbit count verified to \ (0. 01 \) bits at \ (w=3, 7, 8, 9 \). A quantum extension to measurement-induced phase transitions empirically gives finite \ (K^* \) near the area-law phase. v3 changelog: Corrected w=6 boundary case. Previous versions stated j=3 ghost sector inactive at w=6; 20 independent Monte Carlo runs (L=256+512) show partial activation ω₃ = 0. 415 ± 0. 033 (13. 3σ above zero). The ghost condition 4=0 kills the linear Markov trace but NOT the quadratic collision probability. v4: revised framing (Hᵣ2 non-trivial content = value not boundedness), Theorem→Proposition, birthday probability formula for Δ∈0, 1, DLR corollary for A1
Xinlei Wang (Sun,) studied this question.