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Equation 103 · Part 3 · The Bit Comes Back Before the Bearing

Symbol f_1

FQ(t)  ≈  f1 tβ,tG(δ)  ≈  βf1 δ2.F_Q(t) \;\approx\; f_1\,\frac{t}{\beta}, \qquad t_G(\delta) \;\approx\; \frac{\beta}{f_1\,\delta^2}.
f1f_1

What this part means

the per-probe fisher information.

Its job in the formula

f1f_1 occurs below the fraction bar. The quantity above the bar is divided by this expression; zero is excluded as a denominator.

Where the article explains it

This is the standard-quantum-limit regime of parameter estimation: for N independent, identically prepared probes each with per-probe Fisher information f1f_1 , the achievable variance scales as 1/(N f1f_1) , in contrast to the quadratically better Heisenberg scaling available only when probes are used coherently together [ 13 ] .

The passage around this formula

…like an independent sample rather than like a decoded codeword. This is the standard-quantum-limit regime of parameter estimation: for N independent, identically prepared probes each with per-probe Fisher information f1f_1 , the achievable variance scales as 1/(N f1f_1) , in contrast to the quadratically better Heisenberg scaling available only when probes are used coherently together [ 13 ] . Modeling the collected radiation up to time t as contributing Nγ(t)N_\gamma(t) ∼\sim t/β\beta roughly independent quanta gives, as…

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