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Equation 76 · Part 3 · No Particle Without a Cosigner

Symbol c

pa(Ω)=ca g(u),g(u)=24 ue2πu−1,u=cΩa.p_a(\Omega) = \frac{c}{a}\, g(u), \qquad g(u) = \frac{24\,u}{e^{2\pi u}-1}, \qquad u = \frac{c\Omega}{a}.
cc

What this part means

c occurs above the fraction bar. The numerator is divided by the entire denominator below it.

Its job in the formula

c occurs above the fraction bar. The numerator is divided by the entire denominator below it.

The passage around this formula

Write the normalized accelerated spectrum in terms of the dimensionless ratio u ≡\equiv cΩ\Omega/a , using the exact Bose-Einstein shape derived above. Carrying out the normalization integral, ∫0∞\int_0^\infty Ω\Omega\,(e2πcΩ/ae^{2\pi c\Omega/a}-1)^{-1}\,dΩ\Omega = a2a^2/(24c2c^2) , using the standard result ∫0∞\int_0^\infty x(exe^x-1)^{-1}dx=π2\pi^2/6 , gives the scale-family form pa(Ω)=ca g(u),g(u)=24 ue2πu−1,u=cΩap_a(\Omega) = \frac{c}{a}\, g(u), \qquad g(u) = \frac{24\,u}{e^{2\pi u}-1}, \qquad u = \frac{c\Omega}{a}. Every accelerated detector’s normalized spectrum is the same universal curve g , only rescaled by a/c . For two accelerations separated by a small increment, a and a+δ\delta a , standard calculus for a scale family gives, to leading order in δ\delta a ,

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