TY - JOUR
T1 - Explanation for the Absence of Secondary Peaks in Black Hole Light Curve Autocorrelations
AU - Cárdenas-Avendano, Alejandro
AU - Gammie, Charles
AU - Lupsasca, Alexandru
N1 - We thank Maciek Wielgus and George Wong for their valuable comments, and for providing the data for the Sgr and GRMHD light curves, respectively. We also thank Neal Dalal, Suvendu Giri, Lennox Keeble, Aviad Levis, Leo Stein, and Sam Gralla for helpful discussions. C.\u2009G. and A.\u2009L. also thank the Aspen Center for Physics, which is supported by NSF Grant PHY-2210452. A.\u2009C.\u2009A. acknowledges support from the Simons Foundation. A.\u2009L. is supported by NSF Grants AST-2307888 and PHY-2340457. C.\u2009G. was supported in part by the IBM Einstein Fellow Fund at the Institute for Advanced Study. Some of the simulations presented in this work were performed on computational resources managed and supported by Princeton Research Computing, a consortium of groups including the Princeton Institute for Computational Science and Engineering (PICSciE) and the Office of Information Technology\u2019s High Performance Computing Center and Visualization Laboratory at Princeton University.
PY - 2024/9/27
Y1 - 2024/9/27
N2 - The observed radiation from hot gas accreting onto a black hole depends on both the details of the flow and the spacetime geometry. The lensing behavior of a black hole produces a distinctive pattern of autocorrelations within its photon ring that encodes its mass, spin, and inclination. In particular, the time autocorrelation of the light curve is expected to display a series of peaks produced by light echoes of the source, with each peak delayed by the characteristic time lapse τ between light echoes. However, such peaks are absent from the light curves of observed black holes. Here, we develop an analytical model for such light curves that demonstrates how, even though light echoes always exist in the signal, they do not produce autocorrelation peaks if the characteristic correlation timescale λ0 of the source is greater than τ. We validate our model against simulated light curves of a stochastic accretion model ray traced with a general-relativistic code, and then fit the model to an observed light curve for Sgr A∗. We infer that λ0>τ, providing an explanation for the absence of light echoes in the time autocorrelations of Sgr A∗ light curves. Our results highlight the importance for black hole parameter inference of spatially resolving the photon ring via future space-based interferometry.
AB - The observed radiation from hot gas accreting onto a black hole depends on both the details of the flow and the spacetime geometry. The lensing behavior of a black hole produces a distinctive pattern of autocorrelations within its photon ring that encodes its mass, spin, and inclination. In particular, the time autocorrelation of the light curve is expected to display a series of peaks produced by light echoes of the source, with each peak delayed by the characteristic time lapse τ between light echoes. However, such peaks are absent from the light curves of observed black holes. Here, we develop an analytical model for such light curves that demonstrates how, even though light echoes always exist in the signal, they do not produce autocorrelation peaks if the characteristic correlation timescale λ0 of the source is greater than τ. We validate our model against simulated light curves of a stochastic accretion model ray traced with a general-relativistic code, and then fit the model to an observed light curve for Sgr A∗. We infer that λ0>τ, providing an explanation for the absence of light echoes in the time autocorrelations of Sgr A∗ light curves. Our results highlight the importance for black hole parameter inference of spatially resolving the photon ring via future space-based interferometry.
UR - http://www.scopus.com/inward/record.url?scp=85206123145&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=85206123145&partnerID=8YFLogxK
U2 - 10.1103/PhysRevLett.133.131402
DO - 10.1103/PhysRevLett.133.131402
M3 - Article
C2 - 39392980
AN - SCOPUS:85206123145
SN - 0031-9007
VL - 133
JO - Physical review letters
JF - Physical review letters
IS - 13
M1 - 131402
ER -