The QPO in RE J1034+396 Originates in the Hot Corona

RE J1034+396 is one of the few active galactic nuclei (AGNs) with a significant quasiperiodic oscillation (QPO). The QPO has been observed in over 1 Ms of XMM-Newton observations spanning over a decade. We investigate the power spectral density function (PSD) of seven long (∼90 ks) XMM-Newton observ...

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Main Authors: Chloe S. Taylor, Dan R. Wilkins, Steven W. Allen
Format: Article
Language:English
Published: IOP Publishing 2025-01-01
Series:The Astrophysical Journal
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Online Access:https://doi.org/10.3847/1538-4357/ade23d
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author Chloe S. Taylor
Dan R. Wilkins
Steven W. Allen
author_facet Chloe S. Taylor
Dan R. Wilkins
Steven W. Allen
author_sort Chloe S. Taylor
collection DOAJ
description RE J1034+396 is one of the few active galactic nuclei (AGNs) with a significant quasiperiodic oscillation (QPO). The QPO has been observed in over 1 Ms of XMM-Newton observations spanning over a decade. We investigate the power spectral density function (PSD) of seven long (∼90 ks) XMM-Newton observations of the AGN RE J1034+396 in two energy bands. The soft (0.3–0.5 keV) band targets emission from the disk, while the hard (2–7 keV) band isolates the primary X-ray continuum emission from the corona. The QPO is significantly detected in the hard band of five of the seven observations. The best-fitting models indicate that the QPO detection in both bands is entirely attributable to the coronal emission with no additional contribution from the disk. This explains the strong coherence between the hard and soft bands at the QPO frequency. The covariance spectrum is consistent with this picture as the variability at QPO frequencies is attributed solely to fluctuations in the hot corona. The time lag as a function of energy is well described by a ∼2000 s intrinsic soft lag, resulting from the disk responding to emission from the corona, that undergoes phase wrapping at approximately the QPO frequency. By demonstrating that in this system the QPO arises in the corona, we provide new insights into the mechanisms generating QPOs.
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spelling doaj-art-1716b13dffcd4cbf976368c241ee202f2025-08-20T03:31:07ZengIOP PublishingThe Astrophysical Journal1538-43572025-01-01987213510.3847/1538-4357/ade23dThe QPO in RE J1034+396 Originates in the Hot CoronaChloe S. Taylor0https://orcid.org/0000-0003-3117-3476Dan R. Wilkins1https://orcid.org/0000-0002-4794-5998Steven W. Allen2https://orcid.org/0000-0003-0667-5941Department of Physics, Stanford University , 382 Via Pueblo Mall, Stanford, CA 94305, USA ; ctaylor9@stanford.edu, swa@stanford.edu; Kavli Institute for Particle Astrophysics & Cosmology, Stanford University , 452 Lomita Mall, Stanford, CA 94305, USA ; dan.wilkins@stanford.eduKavli Institute for Particle Astrophysics & Cosmology, Stanford University , 452 Lomita Mall, Stanford, CA 94305, USA ; dan.wilkins@stanford.eduDepartment of Physics, Stanford University , 382 Via Pueblo Mall, Stanford, CA 94305, USA ; ctaylor9@stanford.edu, swa@stanford.edu; Kavli Institute for Particle Astrophysics & Cosmology, Stanford University , 452 Lomita Mall, Stanford, CA 94305, USA ; dan.wilkins@stanford.edu; SLAC National Accelerator Laboratory , 2575 Sand Hill Road, Menlo Park, CA 94025, USARE J1034+396 is one of the few active galactic nuclei (AGNs) with a significant quasiperiodic oscillation (QPO). The QPO has been observed in over 1 Ms of XMM-Newton observations spanning over a decade. We investigate the power spectral density function (PSD) of seven long (∼90 ks) XMM-Newton observations of the AGN RE J1034+396 in two energy bands. The soft (0.3–0.5 keV) band targets emission from the disk, while the hard (2–7 keV) band isolates the primary X-ray continuum emission from the corona. The QPO is significantly detected in the hard band of five of the seven observations. The best-fitting models indicate that the QPO detection in both bands is entirely attributable to the coronal emission with no additional contribution from the disk. This explains the strong coherence between the hard and soft bands at the QPO frequency. The covariance spectrum is consistent with this picture as the variability at QPO frequencies is attributed solely to fluctuations in the hot corona. The time lag as a function of energy is well described by a ∼2000 s intrinsic soft lag, resulting from the disk responding to emission from the corona, that undergoes phase wrapping at approximately the QPO frequency. By demonstrating that in this system the QPO arises in the corona, we provide new insights into the mechanisms generating QPOs.https://doi.org/10.3847/1538-4357/ade23dActive galactic nuclei
spellingShingle Chloe S. Taylor
Dan R. Wilkins
Steven W. Allen
The QPO in RE J1034+396 Originates in the Hot Corona
The Astrophysical Journal
Active galactic nuclei
title The QPO in RE J1034+396 Originates in the Hot Corona
title_full The QPO in RE J1034+396 Originates in the Hot Corona
title_fullStr The QPO in RE J1034+396 Originates in the Hot Corona
title_full_unstemmed The QPO in RE J1034+396 Originates in the Hot Corona
title_short The QPO in RE J1034+396 Originates in the Hot Corona
title_sort qpo in re j1034 396 originates in the hot corona
topic Active galactic nuclei
url https://doi.org/10.3847/1538-4357/ade23d
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