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Equation 52 · Part 3 · The Bit Comes Back Before the Bearing

Symbol g

FQ[ρrad(g)]F_Q[\rho_{\mathrm{rad}}(g)]
gg

What this part means

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

Its job in the formula

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

The passage around this formula

which is a genuine constraint, not a simplifying choice: FQF_Q[ρrad(g)\rho_{\mathrm{rad}}(g)] is therefore identical at every point along this orbit, since the quantum Fisher information depends only on the local geometry of the state family under the generator, and a rotated copy of the same family has the same local geometry everywhere. tG(δ)t_G(\delta) does not depend on which heading is being estimated. That is the covariance check this construction owes the reader, and it holds by the same argument that makes the Fisher information of a phase-estimation problem independent of the true phase in ordinary quantum metrology.

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Sources cited in the article section

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