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The spectral evolution of AT 2018dyb and the presence of metal lines in tidal disruption events

Authors :
Leloudas, Giorgos
Dai, Lixin
Arcavi, Iair
Vreeswijk, Paul M.
Mockler, Brenna
Roy, Rupak
Malesani, Daniele B.
Schulze, Steve
Wevers, Thomas
Fraser, Morgan
Ramirez-Ruiz, Enrico
Auchettl, Katie
Burke, Jamison
Cannizzaro, Giacomo
Charalampopoulos, Panos
Chen, Ting-Wan
Cikota, Aleksandar
Della Valle, Massimo
Galbany, Lluis
Gromadzki, Mariusz
Heintz, Kasper E.
Hiramatsu, Daichi
Jonker, Peter G.
Kostrzewa-Rutkowska, Zuzanna
Maguire, Kate
Mandel, Ilya
Onori, Francesca
Nicholl, Matt
Roth, Nathaniel
Smartt, Stephen J.
Wyrzykowski, Lukasz
Young, Dave R.
Leloudas, Giorgos
Dai, Lixin
Arcavi, Iair
Vreeswijk, Paul M.
Mockler, Brenna
Roy, Rupak
Malesani, Daniele B.
Schulze, Steve
Wevers, Thomas
Fraser, Morgan
Ramirez-Ruiz, Enrico
Auchettl, Katie
Burke, Jamison
Cannizzaro, Giacomo
Charalampopoulos, Panos
Chen, Ting-Wan
Cikota, Aleksandar
Della Valle, Massimo
Galbany, Lluis
Gromadzki, Mariusz
Heintz, Kasper E.
Hiramatsu, Daichi
Jonker, Peter G.
Kostrzewa-Rutkowska, Zuzanna
Maguire, Kate
Mandel, Ilya
Onori, Francesca
Nicholl, Matt
Roth, Nathaniel
Smartt, Stephen J.
Wyrzykowski, Lukasz
Young, Dave R.
Publication Year :
2019

Abstract

We present light curves and spectra of the tidal disruption event (TDE) ASASSN-18pg / AT 2018dyb spanning a period of one year. The event shows a plethora of strong emission lines, including the Balmer series, He II, He I and metal lines of O III $\lambda$3760 and N III $\lambda\lambda$ 4100, 4640 (blended with He II). The latter lines are consistent with originating from the Bowen fluorescence mechanism. By analyzing literature spectra of past events, we conclude that these lines are common in TDEs. The spectral diversity of optical TDEs is thus larger than previously thought and includes N-rich events besides H- and He-rich events. We study how the spectral lines evolve with time, by means of their width, relative strength, and velocity offsets. The velocity width of the lines starts at $\sim$ 13000 km s$^{-1}$ and decreases with time. The ratio of He II to N III increases with time. The same is true for ASASSN-14li, which has a very similar spectrum to AT 2018dyb but its lines are narrower by a factor of $>$2. We estimate a black hole mass of $M_{\rm BH}$ = $3.3^{+5.0}_{-2.0}\times 10^6$ $M_{\odot}$ by using the $M$-$\sigma$ relation. This is consistent with the black hole mass derived using the MOSFiT transient fitting code. The detection of strong Bowen lines in the optical spectrum is an indirect proof for extreme ultraviolet and (reprocessed) X-ray radiation and favors an accretion origin for the TDE optical luminosity. A model where photons escape after multiple scatterings through a super-Eddington thick disk and its optically thick wind, viewed at an angle close to the disk plane, is consistent with the observations.<br />Comment: Accepted version. Updated with new photometry and spectra, including an X-shooter spectrum used to determine the BH mass. Two more figures added and line measurements tabulated. No significant scientific updates and the conclusions remain unaffected

Details

Database :
OAIster
Publication Type :
Electronic Resource
Accession number :
edsoai.on1098145753
Document Type :
Electronic Resource
Full Text :
https://doi.org/10.3847.1538-4357.ab5792