2014ApJ...780...44C


Query : 2014ApJ...780...44C

2014ApJ...780...44C - Astrophys. J., 780, 44 (2014/January-1)

The ultraviolet-bright, slowly declining transient PS1-11af as a partial tidal disruption event.

CHORNOCK R., BERGER E., GEZARI S., ZAUDERER B.A., REST A., CHOMIUK L., KAMBLE A., SODERBERG A.M., CZEKALA I., DITTMANN J., DROUT M., FOLEY R.J., FONG W., HUBER M.E., KIRSHNER R.P., LAWRENCE A., LUNNAN R., MARION G.H., NARAYAN G., RIESS A.G., ROTH K.C., SANDERS N.E., SCOLNIC D., SMARTT S.J., SMITH K., STUBBS C.W., TONRY J.L., BURGETT W.S., CHAMBERS K.C., FLEWELLING H., HODAPP K.W., KAISER N., MAGNIER E.A., MARTIN D.C., NEILL J.D., PRICE P.A. and WAINSCOAT R.

Abstract (from CDS):

We present the Pan-STARRS1 discovery of the long-lived and blue transient PS1-11af, which was also detected by Galaxy Evolution Explorer with coordinated observations in the near-ultraviolet (NUV) band. PS1-11af is associated with the nucleus of an early type galaxy at redshift z = 0.4046 that exhibits no evidence for star formation or active galactic nucleus activity. Four epochs of spectroscopy reveal a pair of transient broad absorption features in the UV on otherwise featureless spectra. Despite the superficial similarity of these features to P-Cygni absorptions of supernovae (SNe), we conclude that PS1-11af is not consistent with the properties of known types of SNe. Blackbody fits to the spectral energy distribution are inconsistent with the cooling, expanding ejecta of a SN, and the velocities of the absorption features are too high to represent material in homologous expansion near a SN photosphere. However, the constant blue colors and slow evolution of the luminosity are similar to previous optically selected tidal disruption events (TDEs). The shape of the optical light curve is consistent with models for TDEs, but the minimum accreted mass necessary to power the observed luminosity is only ∼0.002 M☉, which points to a partial disruption model. A full disruption model predicts higher bolometric luminosities, which would require most of the radiation to be emitted in a separate component at high energies where we lack observations. In addition, the observed temperature is lower than that predicted by pure accretion disk models for TDEs and requires reprocessing to a constant, lower temperature. Three deep non-detections in the radio with the Very Large Array over the first two years after the event set strict limits on the production of any relativistic outflow comparable to Swift J1644+57, even if off-axis.

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Journal keyword(s): accretion, accretion disks - black hole physics - galaxies: nuclei

Simbad objects: 17

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Number of rows : 17
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 SN 2007pk SN* 01 31 47.07 +33 36 54.1     17.0     SNIInpec 44 1
2 SN 2011kg SN* 01 39 45.51 +29 55 27.0           SLSN-I 73 1
3 CPD-69 177 WD* 03 10 31.0195960176 -68 36 03.380768388 10.757 11.413 11.394 11.47 11.558 DA3.0 299 0
4 PS1-10bzj SN* 03 31 39.826 -27 47 42.17           SLSN-I 55 0
5 SN 2010jl SN* 09 42 53.33 +09 29 41.8           SNIIn 350 1
6 PS1-11af ev 09 57 26.815 +03 14 01.00           ~ 71 0
7 SDSS J095726.82+031400.9 G 09 57 26.821 +03 14 00.94           ~ 3 0
8 QSO J1024-0052 QSO 10 24 29.58673120 -00 52 55.4963770   18.52 18.35     ~ 143 1
9 SN 2010gx SN* 11 25 46.71 -08 49 41.4           SLSN-I 165 1
10 SN 2008es SN* 11 56 49.13 +54 27 25.7           SNIIL 122 1
11 3C 286 Sy1 13 31 08.2883506368 +30 30 32.960091564   17.51 17.25     ~ 4558 2
12 [DAB2006b] J143227.42+333225.1 SN* 14 32 27.395 +33 32 24.83           SLSN-I 116 0
13 PTF 10iya SN* 14 38 41.00 +37 39 33.6           ~ 33 0
14 PS1-10jh ev 16 09 28.296 +53 40 23.52           ~ 153 0
15 PTF 09cnd SN* 16 12 08.94 +51 29 16.1           SLSN-I 120 0
16 SWIFT J164449.3+573451 G 16 44 47.81184000 +57 35 00.7113480           ~ 533 0
17 SWIFT J2058.4+0516 X 20 58 19.898 +05 13 32.25           ~ 169 0

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