Fig. 19.

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Estimation of the mass of the reprocessing gas responsible for the emission of the spectral lines in TDEs in order to investigate if the recombination time (τrec ≈ (neαB)−1, where ne is the electron density and αB is the case B recombination coefficient) could be responsible for the lags that we discover. We assume its geometrical shape is a sphere (as the simplest approximation) and that the material’s composition is solar-like and fully ionized. We perform three calculations with varying electron densities (which could result to the observed tlags) that in turn yield three total number densities ntot. For all the cases we get a sensible fraction of a solar mass (2.5−10%) assuming the radius of the line emitting region is on the order of 1016 cm.
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