Astronomy and Astrophysics · 2018 · 781 citations · 62 references
Black Hole DynamicRelativistic AstrophysicsPhotometryStar S2EngineeringGeneral RelativityPhysicsBlack Hole PhysicsNatural SciencesBlack HoleAstrodynamicsDirect DetectionGravitational WaveGravitational FieldOrbital SpeedObservational CosmologyGravitational RedshiftAstrophysics
The 16‑year, highly elliptical orbit of S2 around Sgr A* provides a sensitive probe of the Galactic centre’s gravitational field, with pericentre speeds (~7,650 km s⁻¹) making first‑order relativistic effects detectable. Over 26 years the authors monitored S2’s radial velocity and sky motion using VLT’s SINFONI, NACO, and, from 2016 onward, the GRAVITY interferometer. They detected the combined gravitational redshift and transverse Doppler shift (z≈200 km s⁻¹ / c), yielding a post‑Newtonian factor f = 0.90 ± 0.09 (stat) ± 0.15 (sys), inconsistent with pure Newtonian dynamics.
The highly elliptical, 16-year-period orbit of the star S2 around the massive black hole candidate Sgr A ✻ is a sensitive probe of the gravitational field in the Galactic centre. Near pericentre at 120 AU ≈ 1400 Schwarzschild radii, the star has an orbital speed of ≈7650 km s −1 , such that the first-order effects of Special and General Relativity have now become detectable with current capabilities. Over the past 26 years, we have monitored the radial velocity and motion on the sky of S2, mainly with the SINFONI and NACO adaptive optics instruments on the ESO Very Large Telescope, and since 2016 and leading up to the pericentre approach in May 2018, with the four-telescope interferometric beam-combiner instrument GRAVITY. From data up to and including pericentre, we robustly detect the combined gravitational redshift and relativistic transverse Doppler effect for S2 of z = Δ λ / λ ≈ 200 km s −1 / c with different statistical analysis methods. When parameterising the post-Newtonian contribution from these effects by a factor f , with f = 0 and f = 1 corresponding to the Newtonian and general relativistic limits, respectively, we find from posterior fitting with different weighting schemes f = 0.90 ± 0.09| stat ± 0.15| sys . The S2 data are inconsistent with pure Newtonian dynamics.
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