Title. Projection Obstruction for Factorized States: Local Correlation Lower Bounds, Additive Diagnostics, and Observer Recovery Abstract. For a finite quantum system with a time-independent Hamiltonian containing one- and two-site interactions and a product initial state, we bound the departure of each exact two-site reduced state from the product of its own marginals. Define Fe(t)=ρe(t)−ρa(t)⊗ρb(t),De(t)=∥Fe(t)∥1,F_e(t)=ρ_e(t)-ρ_a(t)⊗ρ_b(t), D_e(t)=\|F_e(t)\|_1, where e={a,b}e=\{a,b\} and ∥⋅∥1\|·\|_1 is the full trace norm. With local interaction norm g=maxv∑X∋v∥hX∥∞g=max_v∑X v\|h_X\|_∞ and first-order coefficient νe=∥Fe′(0)∥1ν_e=\|F_e'(0)\|_1, the bound is De(t)≥νet−24g2t2.D_e(t)≥ν_et-24g^2t^2. More generally, if Fe(j)(0)=0F_e⁽ʲ⁾(0)=0 for 0≤j<k0≤ j
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JEREMY H. CARROLL (2026) studied this question.
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