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Equation 100 · A Reference Frame Becomes Classical by Publishing Its Orientation

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pϵ(F)p_\epsilon(F)

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pϵp_\epsilon

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FF

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A fourth rival is more corrosive than the first three because it does not challenge the definitions; it challenges whether they require quantum mechanics at all. Nothing in ρF(g)\rho_F(g) , pϵ(F)p_\epsilon(F) , or Rϵ,δR_{\epsilon,\delta} forces the fragments to be quantum-correlated in a way a classical broadcast could not reproduce. Replace the spin- j rotor with a single classical variable drawn once from the same prior and handed to N independent classical sensors, each corrupted by rotation-equivariant noise tuned to match the quantum construction’s per-fragment error rate. That model satisfies the covariance requirement, clears the blind-guess bound, and can be dialed to any Rϵ,δ(g)R_{\epsilon,\delta}(g)…
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A fourth rival is more corrosive than the first three because it does not challenge the definitions; it challenges whether they require quantum mechanics at all. Nothing in ρF(g)\rho_F(g) , pϵ(F)p_\epsilon(F) , or Rϵ,δR_{\epsilon,\delta} forces the fragments to be quantum-correlated in a way a classical broadcast could not reproduce. Replace the spin- j rotor with a single classical variable drawn once from the same prior and handed to N independent classical sensors, each corrupted by rotation-equivariant noise tuned to match the quantum construction’s per-fragment error rate. That model satisfies the covariance requirement, clears the blind-guess bound, and can be dialed to any Rϵ,δ(g)R_{\epsilon,\delta}(g) the quantum calculation might report, simply by choosing the classical noise level. If a classical dial can always be tuned to impersonate the quantum score, the score is not evidence that a quantum frame became classical; it is a redundancy count that classical estimation theory already understood, dressed in Hilbert-space notation.

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