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Published equation contexts

FQ(t)  ≈  f1 tβ,tG(δ)  ≈  βf1 δ2F_Q(t) \;\approx\; f_1\,\frac{t}{\beta}, \qquad t_G(\delta) \;\approx\; \frac{\beta}{f_1\,\delta^2}

Why this formula appears here

a standard identity in quantum metrology [ 12 ] . Before scrambling, this is fixed by how the compass itself was built — a large, well-prepared gyroscope has a large charge variance and a small intrinsic uncertainty on its own heading. After scrambling, that fixed total has to be reconstructed piecemeal from radiation, and each individually emitted quantum, to the extent it is only weakly and independently correlated with g once the hole’s own state is traced over, contributes an addition to the total that adds 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…

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FQF_Q

Symbol F_Q

FQF_Q is a part of this expression. Its role is fixed by the surrounding article and by the operations shown in the formula.

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tt

Symbol t

t is a part of this expression. Its role is fixed by the surrounding article and by the operations shown in the formula.

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β\beta

Symbol β

β is a part of this expression. Its role is fixed by the surrounding article and by the operations shown in the formula.

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tGt_G

Symbol t_G

tGt_G is a part of this expression. Its role is fixed by the surrounding article and by the operations shown in the formula.

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δ\delta

Symbol delta

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

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δ2\delta^2

Symbol delta^2

delta2a^2 occurs below the fraction bar. The quantity above the bar is divided by this expression; zero is excluded as a denominator.

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f1 δ2f_1\,\delta^2

Denominator: f_1delta^2

The complete quantity below the fraction bar; it must be nonzero for this division.

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How to interpret it

With a fixed numerator, increasing a nonzero denominator reduces the fraction. Its accuracy depends on the assumptions and range of use described in the article.

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Published contexts (1)

A symbol can carry a different meaning in another article. Each occurrence keeps its own guide and term definitions.

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}.

Equation 103 · Evolutionary Physics

The Bit Comes Back Before the Bearing

This equation gives an approximation: it relates the quantities while allowing an approximation.

a standard identity in quantum metrology [ 12 ] . Before scrambling, this is fixed by how the compass itself was built — a large, well-prepared gyroscope has a large charge variance and a small intrinsic uncertainty on its own heading. After scrambling, that fixed total has to be reconstructed piecemeal from radiation, and each individually emitted quantum, to the extent it is only weakly and independently correlated with g once the hole’s own state is traced over, contributes an addition to the total that adds 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…

Meanings in this article

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