Abstract

Context.The density of the ambient medium around a supermassive black hole (SMBH) and the way it varies with distance plays an important role in our understanding of the inflow-outflow mechanisms in the Galactic centre (GC). This dependence is often fitted by spherical power-law profiles based on observations in the X-ray, infrared (IR), submillimetre (submm), and radio domains.Aims.Nevertheless, the density profile is poorly constrained at the intermediate scales of 1000 Schwarzschild radii (Rs). Here we independently constrain the spherical density profile using the stellar bow shock of the star S2 which orbits the SMBH at the GC with the pericentre distance of 14.4 mas (∼1500 Rs).Methods.Assuming an elliptical orbit, we apply celestial mechanics and the theory of bow shocks that are at ram pressure equilibrium. We analyse the measured IR flux density and magnitudes of S2 in theL′-band (3.8 micron) obtained over seven epochs in the years between 2004–2018. We put an upper limit on the emission from S2’s associated putative bow shock and constrain the density profile of the ambient medium.Results.We detect no significant change in S2 flux density until the recent periapse in May 2018. The intrinsic flux variability of S2 is at the level of 2–3%. Based on the dust-extinction model, the upper limit on the number density at the S2 periapse is ∼1.87 × 109 cm−3, which yields a density slope of at most 3.20. Using the synchrotron bow-shock emission, we obtain the ambient density of ≲1.01 × 105 cm−3and a slope of ≲1.47. These values are consistent with a wide variety of media from hot accretion flows to potentially colder and denser media comparable in properties to broad-line-region clouds. However, a standard thin disc can be excluded at the distance of S2’s pericentre.Conclusions.With the current photometry sensitivity of 0.01 mag, we are not able to make stringent constraints on the density of the ambient medium in the GC using S2-star observations. We can distinguish between hot accretion flows and thin, cold discs, where the latter can be excluded at the scale of the S2 periapse. Future observations of stars in the S cluster using instruments such as Mid-IR Extremely Large Telescope Imager and Spectrograph at Extremely Large Telescope with the photometric sensitivity of as much as 10−3mag will allow the GC medium to be probed at intermediate scales at densities as low as ∼700 cm−3in case of non-thermal bow-shock emission. The new instrumentation, in combination with discoveries of stars with smaller pericentre distances, will help to independently constrain the density profile around Sagittarius A* (Sgr A*).

Highlights

  • The Galactic centre (GC) is a unique astrophysical setting where one can study the dynamical effects in one of the densest stellar clusters (Alexander 2005; Merritt 2013; Schödel et al 2014) and the mutual interaction of stars, gaseous-dusty structures, the magnetic field, and the supermassive black hole (SMBH; Genzel et al 2010; Eckart et al 2017)

  • We can distinguish between hot accretion flows and thin, cold discs, where the latter can be excluded at the scale of the S2 periapse

  • The data were obtained from the IR camera Coude NIR Camera (CONICA) and the Nasmyth Adaptive Optics System (NAOS) adaptive optics (AO) module, known as NACO

Read more

Summary

Introduction

The Galactic centre (GC) is a unique astrophysical setting where one can study the dynamical effects in one of the densest stellar clusters (Alexander 2005; Merritt 2013; Schödel et al 2014) and the mutual interaction of stars, gaseous-dusty structures, the magnetic field, and the supermassive black hole (SMBH; Genzel et al 2010; Eckart et al 2017). Ginsburg et al (2016) estimated that the synchrotron emission from S-star bow shocks can be comparable to the Sgr A* radio (10 GHz) and IR flux densities (1014 GHz) for rather extreme combinations of the wind mass-loss rate and its terminal velocity – (mw, vw) = (10−5 M yr−1, 103 km s−1) and (mw, vw) = (10−6 M yr−1, 4 × 103 km s−1) These values deviate from those inferred for S2 (Martins et al 2008; Habibi et al 2017): (mw, vw) = (< 3 × 10−7 M yr−1, 103 km s−1).

Observations and data reduction
Photometry
Photometry results
Extinction estimate inside the Bondi radius
Constraining the ambient density based on the thermal bow-shock emission
Constraining the ambient density based on the non-thermal bow-shock emission
Discussion
Conclusions
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call