NuSTAR Observations of Intrinsically X-Ray Weak Quasar Candidates: An Obscuration-only Scenario

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dc.contributor.authorWang, Chaojun
dc.contributor.authorLuo, B.
dc.contributor.authorBrandt, W. N.
dc.contributor.authorAlexander, D. M.
dc.contributor.authorBauer, F. E.
dc.contributor.authorGallagher, S. C.
dc.contributor.authorHuang, Jian
dc.contributor.authorLiu, Hezhen
dc.contributor.authorStern, D.
dc.date.accessioned2025-01-20T21:02:47Z
dc.date.available2025-01-20T21:02:47Z
dc.date.issued2022
dc.description.abstractWe utilize recent NuSTAR observations (co-added depth approximate to 55-120 ks) of PG 1001+054, PG 1254+047, and PHL 1811 to constrain their hard X-ray (greater than or similar to 5 keV) weakness and spectral shapes and thus to investigate the nature of their extreme X-ray weakness. These quasars showed very weak soft X-ray emission, and they were proposed to be intrinsically X-ray weak, with the X-ray coronae producing weak continuum emission relative to their optical/UV emission. However, the new observations suggest an alternative explanation. The NuSTAR 3-24 keV spectral shapes for PG 1001+054 and PHL 1811 are likely flat (effective power-law photon indices Gamma(eff )= 1.0(-0.6)(+0.5) and Gamma(eff )= 1.4(-0.7)(+0.8) respectively), while the shape is nominal for PG 1254+047 ( Gamma(eff) = 1.8 +/- 0.3). PG 1001+054 and PHL 1811 are significantly weak at hard X-ray energies (by factors of approximate to 26-74 at rest-frame 8 keV) compared to the expectations from their optical/UV emission, while PG 1254+047 is only hard X-ray weak by a factor of approximate to 3. We suggest that X-ray obscuration is present in all three quasars. We propose that, as an alternative to the intrinsic X-ray weakness + X-ray obscuration scenario, the soft and hard X-ray weakness of these quasars can be uniformly explained under an obscuration-only scenario. This model provides adequate descriptions of the multiepoch soft and hard X-ray data of these quasars, with variable column density and leaked fraction of the partial covering absorber. We suggest that the absorber is the clumpy dust-free wind launched from the accretion disk. These quasars probably have super-Eddington accretion rates that drive powerful and high-density winds.
dc.fuente.origenWOS
dc.identifier.doi10.3847/1538-4357/ac886e
dc.identifier.eissn1538-4357
dc.identifier.issn0004-637X
dc.identifier.urihttps://doi.org/10.3847/1538-4357/ac886e
dc.identifier.urihttps://repositorio.uc.cl/handle/11534/93083
dc.identifier.wosidWOS:000850355800001
dc.issue.numero2
dc.language.isoen
dc.revistaAstrophysical journal
dc.rightsacceso restringido
dc.titleNuSTAR Observations of Intrinsically X-Ray Weak Quasar Candidates: An Obscuration-only Scenario
dc.typeartículo
dc.volumen936
sipa.indexWOS
sipa.trazabilidadWOS;2025-01-12
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