TY - JOUR
T1 - Echo mapping of the black hole accretion flow in NGC 7469
AU - Prince, Raj
AU - Hernández Santisteban, Juan V.
AU - Horne, Keith
AU - Gelbord, J.
AU - McHardy, Ian
AU - Edelson, R.
AU - Onken, C. A.
AU - Donnan, F. R.
AU - Vestergaard, M.
AU - Kaspi, S.
AU - Winkler, H.
AU - Cackett, E. M.
AU - Landt, H.
AU - Barth, A. J.
AU - Treu, T.
AU - Valenti, S.
AU - Lira, P.
AU - Chelouche, D.
AU - Romero Colmenero, E.
AU - Goad, M. R.
AU - Gonzalez-Buitrago, D. H.
AU - Kara, E.
AU - Villforth, Carolin
N1 - Funding: R. Prince is grateful for a visiting fellowship funded by the Scottish Universities Physics Alliance (SUPA). The project is partially supported by the Polish Funding Agency National Science Centre, project 2017/26/A/ST9/-00756 (MAESTRO 9) and the European Research Council (ERC) under the European Union’s Horizon 2020 research and innovation program (grant agreement No. 951549) and BHU IoE scheme. HL acknowledges a Daphne Jackson Fellowship sponsored by the Science and Technology Facilities Council (STFC), UK.
PY - 2025/7/4
Y1 - 2025/7/4
N2 - Reverberation mapping (RM) can measure black hole accretion disc sizes and radial structure through observable light travel time lags that should increase with wavelength as τ ∝ λ4/3 due to the disc’s T ∝ r−3/4 temperature profile. Our 250-d RM campaign on NGC 7469 combines sub-day cadence 7-band photometry from the Las Cumbres Observatory robotic telescopes and weekly X-ray and UVOT data from Swift. By fitting these light curves, we measure the spectral energy distribution (SED) of the variable accretion disc, and inter-band lags of just 1.5 d across the UV to optical range. The disc SED is close to the expected fν ∝ ν1/3, and the lags are consistent with τ ∝ λ4/3, but three times larger than expected. We consider several possible modifications to standard disc assumptions. First, for a 9 × 106 M☉ black hole and two possible spins a* = (0, 1), we fit the X-ray-ultraviolet (UV)-optical SED with a compact relativistic corona at height Hx ∼ (46, 27) Rg irradiating a flat disc with accretion rate ṁEdd ∼ (0.23, 0.24) inclined to the line of sight by i < 20°. To fit the lags as well as the SED, this model requires a low spin a* ≈ 0 and boosts disc colour temperatures by a factor fcol ≈ 1.8, which shifts reprocessed light to shorter wavelengths. Our Bowl model with fcol = 1 neglects relativity near the black hole, but fits the UV-optical lags and SEDs using a flat disc with ṁEdd < 0.06 and a steep outer rim at Rout/c ∼ 5 − 10 d with H/R < 1 per cent. This rim occurs near the 103K dust sublimation temperature in the disc atmosphere, supporting models that invoke dust opacity to thicken the disc and launch failed radiatively driven dusty outflows at the inner edge of the broad line region (BLR). Finally, the disc lags and SEDs exhibit a significant excess in the u and r bands, suggesting Balmer continuum and Hα emission, respectively, from the BLR.
AB - Reverberation mapping (RM) can measure black hole accretion disc sizes and radial structure through observable light travel time lags that should increase with wavelength as τ ∝ λ4/3 due to the disc’s T ∝ r−3/4 temperature profile. Our 250-d RM campaign on NGC 7469 combines sub-day cadence 7-band photometry from the Las Cumbres Observatory robotic telescopes and weekly X-ray and UVOT data from Swift. By fitting these light curves, we measure the spectral energy distribution (SED) of the variable accretion disc, and inter-band lags of just 1.5 d across the UV to optical range. The disc SED is close to the expected fν ∝ ν1/3, and the lags are consistent with τ ∝ λ4/3, but three times larger than expected. We consider several possible modifications to standard disc assumptions. First, for a 9 × 106 M☉ black hole and two possible spins a* = (0, 1), we fit the X-ray-ultraviolet (UV)-optical SED with a compact relativistic corona at height Hx ∼ (46, 27) Rg irradiating a flat disc with accretion rate ṁEdd ∼ (0.23, 0.24) inclined to the line of sight by i < 20°. To fit the lags as well as the SED, this model requires a low spin a* ≈ 0 and boosts disc colour temperatures by a factor fcol ≈ 1.8, which shifts reprocessed light to shorter wavelengths. Our Bowl model with fcol = 1 neglects relativity near the black hole, but fits the UV-optical lags and SEDs using a flat disc with ṁEdd < 0.06 and a steep outer rim at Rout/c ∼ 5 − 10 d with H/R < 1 per cent. This rim occurs near the 103K dust sublimation temperature in the disc atmosphere, supporting models that invoke dust opacity to thicken the disc and launch failed radiatively driven dusty outflows at the inner edge of the broad line region (BLR). Finally, the disc lags and SEDs exhibit a significant excess in the u and r bands, suggesting Balmer continuum and Hα emission, respectively, from the BLR.
KW - Accretion
KW - Accretion discs
KW - Galaxies: active
KW - Galaxies: Seyfert
KW - Galaxies: individual: NGC 7469
UR - https://www.scopus.com/pages/publications/105010215667
U2 - 10.1093/mnras/staf983
DO - 10.1093/mnras/staf983
M3 - Article
SN - 0035-8711
VL - 541
SP - 642
EP - 661
JO - Monthly Notices of the Royal Astronomical Society
JF - Monthly Notices of the Royal Astronomical Society
IS - 1
ER -