The corona contracts in a black-hole transient.

Kara, E; Steiner, J F; Fabian, A C; Cackett, E M; Uttley, P; Remillard, R A; Gendreau, K C; Arzoumanian, Z et al. · Nature · 2019

basic_science · Level V

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Abstract

The geometry of the accretion flow around stellar-mass black holes can change on timescales of days to months<sup>1-3</sup>. When a black hole emerges from quiescence (that is, it 'turns on' after accreting material from its companion) it has a very hard (high-energy) X-ray spectrum produced by a hot corona<sup>4,5</sup> positioned above its accretion disk, and then transitions to a soft (lower-energy) spectrum dominated by emission from the geometrically thin accretion disk, which extends to the innermost stable circular orbit<sup>6,7</sup>. Much debate persists over how this transition occurs and whether it is driven largely by a reduction in the truncation radius of the disk<sup>8,9</sup> or by a reduction in the spatial extent of the corona<sup>10,11</sup>. Observations of X-ray reverberation lags in supermassive black-hole systems<sup>12,13</sup> suggest that the corona is compact and that the disk extends nearly to the central black hole<sup>14,15</sup>. Observations of stellar-mass black holes, however, reveal equivalent (mass-scaled) reverberation lags that are much larger<sup>16</sup>, leading to the suggestion that the accretion disk in the hard-X-ray state of stellar-mass black holes is truncated at a few hundreds of gravitational radii from the black hole<sup>17,18</sup>. Here we report X-ray observations of the black-hole transient MAXI J1820+070<sup>19,20</sup>. We find that the reverberation time lags between the continuum-emitting corona and the irradiated accretion disk are 6 to 20 times shorter than previously seen. The timescale of the reverberation lags shortens by an order of magnitude over a period of weeks, whereas the shape of the broadened iron K emission line remains remarkably constant. This suggests a reduction in the spatial extent of the corona, rather than a change in the inner edge of the accretion disk.