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Unmodeled brightness excess in WR 20a’s B and V light curves near phases 0.1–0.3

Explain and accurately model the observed higher flux at orbital phases 0.1–0.3 compared to phases 0.6–0.8 in the B and V light curves of the eclipsing binary WR 20a, which neither the standard Roche model nor the steady-state colliding-wind model currently reproduces.

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Background

While the colliding-wind model presented in the paper successfully captures the overall light-curve asymmetry due to the inclined wind–wind interaction zone, the authors highlight a specific discrepancy: an elevated brightness at phases 0.1–0.3 relative to 0.6–0.8 in B and V that their steady-state model (and the standard Roche model) does not fit.

They suggest non-stationary processes in the wind–wind collision zone may account for this effect, noting that averaged TESS and ASAS-SN data do not show the same excess. However, an explicit physical explanation and a model that reproduces this feature remain outstanding.

References

However, neither the standard Roche model used in nor our model can accurately describe the observational light curves (at least in the $BV$ filters) in the phase range \mbox{0.1--0.3}, where the observational light curves are higher than at the similar phases after the secondary minimum \mbox{0.6--0.8}. We will return to this issue below.

The massive binary system WR 20a: light curve analysis in a colliding wind model (2510.16902 - Antokhin et al., 19 Oct 2025) in Section 3, Analysis and results