Constructs a battery-explicit thermodynamic witness that converts Bell-game success probabilities into ceilings on mean battery charge, with Tsirelson's bound as the quantum limit for CHSH.
ForN= 2, this gives ωQ(G2) = cos2 π 8 , which is the usual CHSH quantum winning probability
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Battery-Explicit Thermodynamic Witnesses of Bell Post-Quantumness
Constructs a battery-explicit thermodynamic witness that converts Bell-game success probabilities into ceilings on mean battery charge, with Tsirelson's bound as the quantum limit for CHSH.