posted on 2025-09-18, 16:00authored byD Gonzalez-Buitrago, AJ Barth, R Edelson, JV Hernández Santisteban, Keith Horne, T Schmidt, Yan-Rong Li, Hengxiao Guo, MD Joner, E Cackett, J Gelbord, MC Bentz, WN Brandt, Michael GoadMichael Goad, K Korista, M Vestergaard, C Villforth, A Breeveld, TG Brink, EM Corsini, E Dalla Bontà, Gary J Ferland, AV Filippenko, Ma T García-Díaz, M Hallum, JC Horst, M Kim, Y Krongold, J Kruger, B Kuhn, S Kumar, M Mehdipour, L Morelli, S Mathur, H Netzer, P Ochner, I Pagotto, A Pizzella, DJ Sand, A Siviero, M Spencer, H Sung, S Vaughan, H Winkler, W Zheng
Abstract
We present ground-based, multi-band light curves of the AGN Mrk 509, NGC 4151, and NGC 4593 obtained contemporaneously with Swiftmonitoring. We measure cross-correlation lags relative to SwiftUVW2 (1928 Å) and test the standard prediction for disk reprocessing, which assumes a geometrically thin, optically thick accretion disk where continuum interband delays follow the relation τ(λ)∝λ4/3. For Mrk 509 the 273-d Swiftcampaign gives well-defined lags that increase with wavelength as τ(λ)∝λ2.17 ± 0.2, steeper than the thin-disk prediction, and the optical lags are a factor of ∼5 longer than expected for a simple disk-reprocessing model. This “disk-size discrepancy” as well as excess lags in the u and r bands (which include the Balmer continuum and Hα, respectively) suggest a mix of short lags from the disk and longer lags from nebular continuum originating in the broad-line region. The shorter Swiftcampaigns, 69 d on NGC 4151 and 22 d on NGC 4593, yield less well-defined, shorter lags <2 d. The NGC 4593 lags are consistent with τ(λ)∝λ4/3 but with uncertainties too large for a strong test. For NGC 4151 the Swiftlags match τ(λ)∝λ4/3, with a small U-band excess, but the ground-based lags in the r, i, and z bands are significantly shorter than the B and g lags, and also shorter than expected from the thin-disk prediction. The interpretation of this unusual lag spectrum is unclear. Overall these results indicate significant diversity in the τ − λ relation across the optical/UV/NIR, which differs from the more homogeneous behavior seen in the Swiftbands.<p></p>
History
Author affiliation
College of Science & Engineering
Physics & Astronomy
Access to the data used in this article is subject to request to the author and will only be provided with the authorization of the Principal Investigators (PIs) of the IBRM project.