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Equation 152 · The Bit Comes Back Before the Bearing

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δ∗\delta^\ast

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δ∗\delta^\ast

Symbol delta^ast

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That experiment has nothing to say about tGt_G . Its seven qubits carry no conserved charge playing the role J^\hat J plays above, no compass was thrown in, and no alignment problem of the kind Bartlett, Rudolph, and Spekkens formalize was ever posed to the circuit [ 9 ] . The honest parameter range this construction can claim, then, is narrow and asymmetric on purpose: the mechanism behind tLt_L has a laboratory analogue at the scale of a handful of trapped ions, verified by an actual measured teleportation fidelity; the mechanism behind tGt_G has none. Every number attached to tGt_G in this article — the toy accumulation law, the per-quantum Fisher information f1f_1 , the crossover tolerance…
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That experiment has nothing to say about tGt_G . Its seven qubits carry no conserved charge playing the role J^\hat J plays above, no compass was thrown in, and no alignment problem of the kind Bartlett, Rudolph, and Spekkens formalize was ever posed to the circuit [ 9 ] . The honest parameter range this construction can claim, then, is narrow and asymmetric on purpose: the mechanism behind tLt_L has a laboratory analogue at the scale of a handful of trapped ions, verified by an actual measured teleportation fidelity; the mechanism behind tGt_G has none. Every number attached to tGt_G in this article — the toy accumulation law, the per-quantum Fisher information f1f_1 , the crossover tolerance δ∗\delta^\ast — is a phenomenological construction consistent with a rigorous symmetry result, not a measured or simulated quantity, and it should be read that way.

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