By studying the optical brightness surface density of the globular cluster NGC 6388, it has been recently proposed that it harbors a central intermediate-mass black hole with mass 5.7×10 3 M . We expect that the compact object in the center of NGC 6388 emits radiation in the X-ray band as a consequence of the accretion from the surrounding matter. We searched for XM M -Newton and Chandra observations towards NGC 6388 to test this hypothesis. The Chandra satellite disentangles several point-like X-ray sources, probably low mass X-ray binaries, well within the core radius of the globular cluster. However, three of them, coinciding with the cluster center of gravity, remain unresolved. Their total luminosity is LObs 2.7 × 1033 erg s−1 . If one of X these sources is the X-ray counterpart of the intermediate-mass black hole in NGC 6388, the corresponding upper limit on the accretion efficiency, with respect to the Eddington luminosity, is 3 × 10−9 . This measurement could be tightened if moderately deep radio observations of the field were performed.
The globular cluster NGC 6388: XMM-Newton and Chandra observations
NUCITA, Achille;DE PAOLIS, Francesco;INGROSSO, Gabriele;
2008-01-01
Abstract
By studying the optical brightness surface density of the globular cluster NGC 6388, it has been recently proposed that it harbors a central intermediate-mass black hole with mass 5.7×10 3 M . We expect that the compact object in the center of NGC 6388 emits radiation in the X-ray band as a consequence of the accretion from the surrounding matter. We searched for XM M -Newton and Chandra observations towards NGC 6388 to test this hypothesis. The Chandra satellite disentangles several point-like X-ray sources, probably low mass X-ray binaries, well within the core radius of the globular cluster. However, three of them, coinciding with the cluster center of gravity, remain unresolved. Their total luminosity is LObs 2.7 × 1033 erg s−1 . If one of X these sources is the X-ray counterpart of the intermediate-mass black hole in NGC 6388, the corresponding upper limit on the accretion efficiency, with respect to the Eddington luminosity, is 3 × 10−9 . This measurement could be tightened if moderately deep radio observations of the field were performed.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.