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Equation 21 · Part 6 · No Particle Without a Cosigner

fraction

px(Ω)=Fx(Ω)∫0∞Fx(Ω′) dΩ′,Ω>0,p_x(\Omega) = \frac{\mathcal F_x(\Omega)}{\displaystyle\int_0^\infty \mathcal F_x(\Omega')\, d\Omega'}, \qquad \Omega > 0,
fraction

What this part means

Divide the expression above the line by the one below it.

Its job in the formula

The expression above the fraction bar is divided by the complete expression below it. The denominator must not be zero.

The passage around this formula

Fx(Ω)\mathcal F_x(\Omega) , viewed as a function of Ω\Omega for fixed everything else, has a natural reading as a spectrum: it says how much excitation probability accumulates at each possible gap, for a whole notional bank of detectors sharing one trajectory, one switching profile, and one field state, differing only in Ω\Omega . Restricting to the excitation branch Ω\Omega>0 — “did this detector behave as though it absorbed a quantum” is the only branch this article treats as bearing on particle content, since the decay branch Ω\Omega<0 mixes genuine field structure with detector-specific spontaneous-emission physics that is present even in flat, empty spacetime with no field excitation at all —…

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Learn the underlying idea

A fraction a/b means a divided by b. The top number is the numerator; the bottom number is the denominator, and it cannot be zero.

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Sources cited in the article section

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