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Equation 89 · No Particle Without a Cosigner

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Ddet(a, a+δa)  ≈  0.394 ∣δa∣a.D_{\rm det}(a,\, a+\delta a) \;\approx\; 0.394\, \frac{|\delta a|}{a}.

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This equation gives an approximation: it relates the quantities while allowing an approximation. Read the equation part by part below; each part has a contextual explanation and a link to its mathematical background.

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DdetD_{\rm det}

Symbol D_rm det

well defined, it can be evaluated, and the cleanest case where it is well defined and non-trivial is a comparison between two accelerated trajectories, both with finite normalizable spectra, differing only slightly in acceleration.

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aa

Symbol a

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

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δ\delta

Symbol delta

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

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fraction

fraction

Divide the expression above the line by the one below it.

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≈

≈

Approximately equal to; the equality is not exact.

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addition

addition

Add the term after the plus sign to the term or group before it.

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subscript

subscript

The lower label selects a particular version, component, or indexed member of the quantity. For example, x₀ and xₜ can be values at different positions.

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∣δa∣|\delta a|

Numerator: |delta a|

The complete quantity above the fraction bar.

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How to interpret it

With a fixed numerator, increasing a nonzero denominator reduces the fraction. Its accuracy depends on the assumptions and range of use described in the article.

What the article says around this equation

This is the same trick used to derive Wien’s displacement law: because u\,g(u) rises from zero, passes through a single interior maximum, and falls back to zero, the integral of the absolute value of its derivative over all u is exactly twice that maximum, with no need to evaluate the integral directly. Finding the maximum of u\,g(u) = 24\,u2u^2/(e2πue^{2\pi u}-1) means solving e2πu(1−πu)e^{2\pi u}(1-\pi u)=1 , the same class of transcendental equation that fixes the peak of a Planck spectrum weighted by an extra power of frequency. Solved by Newton’s method to five-figure precision, the nontrivial root is u∗u^\ast ≈\approx 0.25363 , at which u∗u^\ast g(u∗u^\ast) ≈\approx 0.3937 . The leading-order sensitivity is…
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This is the same trick used to derive Wien’s displacement law: because u\,g(u) rises from zero, passes through a single interior maximum, and falls back to zero, the integral of the absolute value of its derivative over all u is exactly twice that maximum, with no need to evaluate the integral directly. Finding the maximum of u\,g(u) = 24\,u2u^2/(e2πue^{2\pi u}-1) means solving e2πu(1−πu)e^{2\pi u}(1-\pi u)=1 , the same class of transcendental equation that fixes the peak of a Planck spectrum weighted by an extra power of frequency. Solved by Newton’s method to five-figure precision, the nontrivial root is u∗u^\ast ≈\approx 0.25363 , at which u∗u^\ast g(u∗u^\ast) ≈\approx 0.3937 . The leading-order sensitivity is therefore Ddet(a, a+δa)  ≈  0.394 ∣δa∣aD_{\rm det}(a,\, a+\delta a) \;\approx\; 0.394\, \frac{|\delta a|}{a}. Two accelerated worldlines whose accelerations differ by one part in a thousand disagree, on this measure, by about four parts in ten thousand in normalized excitation content — a small number, appropriately, since a one-part-in-a-thousand physical difference should produce a comparably graded disagreement rather than a large one. This is the sense in which the coefficient 0.394 is an exact result: it is the exact leading term of a convergent expansion in δ\delta a/a , obtained from an exact closed-form spectral shape by ordinary calculus, with the only numerical step being the solution of one transcendental equation to a stated precision. It is illustrative, not a report of anything measured, and it says nothing about accelerations that are not small perturbations of one another.

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