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Fig. 5.

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Detection prospects for KNRs from their temporal evolution information. Top: Δ F F Δ t $ \frac{\Delta F}{F\Delta t} $ for our fiducial cases with Δt = 5 yr. dlog F 3 GHz d t $ \frac{\mathrm{dlog}F_{\mathrm{3 GHz}}}{\mathrm{d}t} $ approaches 3/t and ∼1/t in the blast wave and ST regimes, respectively. Bottom: ( Δ F F ) × ( t ST Δ t ) $ (\frac{\Delta F}{F})\times (\frac{t_{\mathrm{ST}}}{\Delta t}) $ for the three cases with Δt = 5 yr. We note that tST is not available to us directly and has to be extracted from the light-curve data. As ( Δ F F ) × ( t ST Δ t ) $ (\frac{\Delta F}{F})\times (\frac{t_{\mathrm{ST}}}{\Delta t}) $ is similar for all cases around the Sedov time, we can estimate tST from observed quantities, such as Δ F F $ \frac{\Delta F}{F} $ and Δt (Eq. (37)). As an example, we show the case for an EKNR for which Δ F F Δ t 0.02 yr 1 $ \frac{\Delta F}{F\Delta t}\sim 0.02\,\mathrm{yr^{-1}} $ at around the time when it starts to enter deep into the Sedov regime (upper panel).

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