Jerome A. Orosz Created 2026-10-20 Updated 2026-11-05
Jerome A. Orosz coauthored a dynamical model of Cygnus X-1 that combines optical light curves, companion-star radial velocities, rotational broadening and a distance constraint to infer the black hole's mass.[ref]
The Mass of the Black Hole in Cygnus X-1 by Jerome A. Orosz and others. Abstract: photometric/spectroscopic constraints and binary model
The measurements constrain different parts of the binary geometry. Radial motion alone leaves an inclination dependence; stellar size and light-curve information help determine the scale and orientation. The quoted paper is a specific historical analysis, so its parameter estimates should not be mistaken for an automatically current calibration.
A donor star can feed a compact companion through Roche-lobe overflow near the inner Lagrange point, or through capture of a stellar wind. The transferred gas usually carries angular momentum; when its circularization radius exceeds the accretor's effective inner radius it forms an accretion disc. Outward angular momentum transport permits inward mass flow, while dissipation converts gravitational binding energy into heat and radiation. For a compact object with a surface ; for a black hole write , with efficiency determined by the flow and inner boundary. Optically thick disc regions emit a sum of thermal radiation spectrum components; a hot optically thin accretion corona can inverse-Compton scatter softer photons into a harder X-ray component. A black hole has no material surface on which to radiate a stellar boundary layer.
An explicit example is the wind-fed black-hole binary Cygnus X-1. Its massive stellar companion supplies gas, and the accretion flow produces strong X-ray emission.[ref]
Wind Accretion and State Transitions in Cygnus X-1 by D. R. Gies and others. abstract, H-alpha wind monitoring and X-ray-state comparison
Compact-object evidence comes from orbital dynamics rather than X-ray brightness alone. The single-lined binary mass function constrains the unseen mass; inclination, donor properties and distance refine it. Jerome A. Orosz and collaborators combined optical photometry, radial velocities, rotation and a distance constraint to obtain a black-hole mass of in their 2011 analysis. The inference depends on the stellar and orbital model, and that historical value should not be confused with a latest measurement.[ref]The Mass of the Black Hole in Cygnus X-1 by Jerome A. Orosz and others. abstract; dynamical modelling and observational constraints
Binary accretion converts orbital mass transfer into compact gravitational-energy release; a dynamical mass measurement identifies the accretor more securely than luminosity alone.