Figure 7.
Simulated light curves (left column) and corresponding rms–flux binned data. Middle column shows the rms–flux data taken from full light curves with linear fits as dashed lines with a being linear coefficients of equation rms = aψ + b (where ψ is the flux). The two lower-right panels show linear fits to individual simulated light-curve subsamples (outbursts). The upper-right square panel is a detail of the upper middle panel. Flux is in arbitrary units (au). A – constant mass accretion rate, B – increasing mass accretion rate with correspondingly increasing number of flickering flares per light-curve subsegment, C – the same as B but with constant flickering flare number per light-curve subsegment and an additional vertical offset is added instead, D and E – the same as B and C, respectively, but light-curve subsegments are randomly redistributed in order to simulate the outbursts. See the text for details.

Simulated light curves (left column) and corresponding rms–flux binned data. Middle column shows the rms–flux data taken from full light curves with linear fits as dashed lines with a being linear coefficients of equation rms = aψ + b (where ψ is the flux). The two lower-right panels show linear fits to individual simulated light-curve subsamples (outbursts). The upper-right square panel is a detail of the upper middle panel. Flux is in arbitrary units (au). A – constant mass accretion rate, B – increasing mass accretion rate with correspondingly increasing number of flickering flares per light-curve subsegment, C – the same as B but with constant flickering flare number per light-curve subsegment and an additional vertical offset is added instead, D and E – the same as B and C, respectively, but light-curve subsegments are randomly redistributed in order to simulate the outbursts. See the text for details.

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