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Equation 46 · Part 1 · No Particle Without a Cosigner

Symbol chi

χ(τ)\chi(\tau)
χ\chi

What this part means

all defined intrinsically along each worldline.

Its job in the formula

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

Where the article explains it

DdetD_{\rm det} also does not change under a Poincaré transformation applied identically to both worldlines and to the field vacuum together, since W is Poincaré invariant and τ\tau , Ω\Omega , and χ\chi are all defined intrinsically along each worldline.

The passage around this formula

…time instead of proper time would inject that redshift directly into DdetD_{\rm det} as a spurious “particle disagreement” that is really just two clocks running at different rates. The fourth is the switching profile χ(τ)\chi(\tau) : its total duration and its smoothness both leave fingerprints in Fx(Ω)\mathcal F_x(\Omega) that have nothing to do with the trajectory, as the next two sections show in detail.

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A function assigns an output to each allowed input. The expression f(x) means “apply f to x”.

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Sources cited in the surrounding passage

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