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Equation 10 · Part 5 · No Particle Without a Cosigner

Symbol chi

Fx(Ω)=∫dτ dτ′ χ(τ)χ(τ′) e−iΩ(τ−τ′) W[x(τ),x(τ′)],\mathcal F_x(\Omega) = \int d\tau\, d\tau'\, \chi(\tau)\chi(\tau')\, e^{-i\Omega(\tau-\tau')}\, W\big[x(\tau), x(\tau')\big],
χ\chi

What this part means

chi is one of the signed contributions combined to compute the quantity on the left.

Its job in the formula

chi is one of the signed contributions combined to compute the quantity on the left.

The passage around this formula

…off a dial. The response functional for a pointlike, linearly coupled two-level (Unruh-DeWitt) detector on worldline x(τ\tau) , parametrized by its own proper time τ\tau , with energy gap Ω\Omega and switching function χ(τ)\chi(\tau) controlling when the interaction is on, is Fx(Ω)=∫dτ dτ′ χ(τ)χ(τ′) e−iΩ(τ−τ′) W[x(τ),x(τ′)]\mathcal F_x(\Omega) = \int d\tau\, d\tau'\, \chi(\tau)\chi(\tau')\, e^{-i\Omega(\tau-\tau')}\, W\big[x(\tau), x(\tau')\big]. where W is the field’s two-point Wightman function evaluated along the trajectory [ 5 ] . Three things in this expression are worth fixing in the reader’s mind before anything else happens to it. First, τ\tau is proper time —…

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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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