AGN STORM 2. XII. Ground-Based Optical Photometry and Lag Measurements of Mrk 817
John W. Montano, Aaron J. Barth, Keith Horne, Edward M. Cackett, Gisella De Rosa + 38 more
TLDR
New optical photometry of Mrk 817 measures reverberation lags, revealing a disk size discrepancy and variations linked to ionizing luminosity changes.
Key contributions
- Measured optical reverberation lags for Mrk 817 over 1.4 years using uBgVriz filters and three methods.
- ICCF lags (3.0-7.9 days) align with a λ^(4/3) Shakura-Sunyaev disk, but other methods differ.
- Observed lags are 3-6 times longer than thin-disk predictions, confirming the "disk size discrepancy."
- Lags vary by up to a factor of two between epochs, linked to changes in ionizing luminosity and obscuration.
Why it matters
This study provides crucial new data on AGN accretion disk structure and variability in Mrk 817. It confirms the persistent "disk size discrepancy" in Seyfert galaxies, and the finding that continuum lags vary with ionizing luminosity offers new insights into how accretion disk properties evolve.
Original Abstract
We present the ground-based imaging campaign and light curves of Markarian 817 as part of the multiwavelength monitoring program AGN STORM\,2. Observations were carried out over 1.4 years in \emph{uBgVriz} filters, with a median cadence of 0.4 days in \emph{g}. Reverberation lags are measured using three methods (ICCF, JAVELIN, and PyROA) with the Swift UVW2 band (1928 Å) as the reference light curve. The ICCF centroid lags range from $3.0\pm0.8$ days for the $u$ band up to $7.9\pm1.5$ days for $z$, and are consistent with a $τ\propto λ^{4/3}$ dependence, the relation expected for lamp-post reprocessing by a Shakura-Sunyaev disk. Lags measured with the other methods are systematically shorter, and deviate from a $λ^{4/3}$ power-law spectrum at long wavelengths. The lags exceed thin-disk reprocessing predictions by factors of $\sim$3-6, similar to the ``disk size discrepancy'' seen in other Seyfert galaxies. We divide the campaign into three epochs with different levels of mean luminosity and X-ray obscuring column density and find that the lags vary by as much as a factor of 2 between epochs. The intrinsic spectral energy distribution is bluer and brighter during the first third of the campaign, and the longest continuum reverberation lags are obtained during that period. These results suggest that changes in ionizing luminosity can produce large variations in continuum lags on short timescales by altering the diffuse continuum luminosity emitted by the broad-line region and/or obscuring outflow, although changes in obscuration between the central engine and broad-line region may also contribute to the lag variations.
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