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Equation 24 · Part 4 · No Particle Without a Cosigner

Symbol d

Ddet(x,y)=12∫0∞dΩ ∣px(Ω)−py(Ω)∣.D_{\rm det}(x,y) = \frac12 \int_0^\infty d\Omega\, \big| p_x(\Omega) - p_y(\Omega) \big|.
dd

What this part means

d is part of the quantity the equation computes from the expression on the right.

Its job in the formula

d is part of the quantity the equation computes from the expression on the right.

The passage around this formula

defined whenever the denominator is finite and nonzero. Given two such normalized spectra, for a detector on worldline x and a detector on worldline y , define their disagreement as the total variation distance between the two probability densities: Ddet(x,y)=12∫0∞dΩ ∣px(Ω)−py(Ω)∣D_{\rm det}(x,y) = \frac12 \int_0^\infty d\Omega\, \big| p_x(\Omega) - p_y(\Omega) \big|. This is the object this article is actually about, so its bookkeeping has to be stated in full before any number is produced. DdetD_{\rm det} is a map from pairs of “treaty configurations” — worldline, field state, coupling type, and the gap/switching pair used to build the spectrum — to the real interval [0,1] ; it carries no physical units, because it is built entirely from normalized probability densities over Ω\Omega , whose…

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Sources cited in the article section

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