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.
Let z= Φ −1 1− α 2 , where Φ is the standard normal cumulative distribution function
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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.