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Equation 35 · Part 1 · No Particle Without a Cosigner

Symbol chi

χ\chi
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

…no freedom here to exploit. 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. What does change DdetD_{\rm det} , and is meant to, is any actual physical difference between the two setups. The discipline this article insists on is separating that meant-to variation from an unmeant one: before attributing a nonzero D_{\rm…

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Sources cited in the article section

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