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Equation 76 · Part 1 · No Particle Without a Cosigner

Symbol p_a

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}.
pap_a

What this part means

pap_a is part of the quantity the equation computes from the expression on the right.

Its job in the formula

pap_a is part of the quantity the equation computes from the expression on the right.

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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