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For the forward ray of i, the ultrarelativistic longitudinal Doppler factor follows from the exact expression in terms of the Lorentz factor:Indeed, $\gamma \beta =\sqrt{{\gamma }^2-1}$ for a positive boost. If $\beta =1-ϵ$, the exact formulas and their consistent asymptotic expansions areEquivalently,The printed equality is not exact. For a concrete ultrarelativistic example, $\gamma =10$ gives the correct $D=10+\sqrt{99}\simeq 19.949874$, whereas $\sqrt{4{\gamma }^2-1}=\sqrt{399}\simeq 19.974984$. The latter expands as $2\gamma -1/(4\gamma )+O({\gamma }^{-3})$, with the wrong first correction.

One can obtain the printed expression by using $D^2=2/ϵ-1$ but replacing ${\gamma }^2$ by only its leading approximation $1/(2ϵ)$. This retains a constant term in the first equation while discarding a same-order term in the second. Thus $D\approx \sqrt{4{\gamma }^2-1}$ is admissible only as a leading relative-accuracy estimate, of the same order as $D\sim 2\gamma$; it is not the stated identity or a correct next-order approximation.