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View details. Flag as inappropriate. He conceded the bet in after observational data had strengthened the case that there was indeed a black hole in the system. This hypothesis lacks direct empirical evidence but has generally been accepted from indirect evidence. Observation of X-ray emissions allows astronomers to study celestial phenomena involving gas with temperatures in the millions of degrees.
However, because X-ray emissions are blocked by the Earth's atmosphere , observation of celestial X-ray sources is not possible without lifting instruments to altitudes where the X-rays can penetrate. As part of an ongoing effort to map these sources, a survey was conducted in using two Aerobee suborbital rockets. These instruments swept across the sky as the rockets rotated, producing a map of closely spaced scans.
The celestial coordinates of this source were estimated as right ascension 19 h 53 m and declination It was not associated with any especially prominent radio or optical source at that position. Seeing a need for longer duration studies, in Riccardo Giacconi and Herb Gursky proposed the first orbital satellite to study X-ray sources.
For a size comparison, the diameter of the Sun is about 1. Miley from Leiden Observatory , and independently Robert M. Measurements of the Doppler shift of the star's spectrum demonstrated the companion's presence and allowed its mass to be estimated from the orbital parameters. This interval is consistent with turbulence in a disk of accreted matter surrounding a black hole—the accretion disk.
X-ray bursts that last for about a third of a second match the expected time frame of matter falling toward a black hole. The compact object and blue supergiant star form a binary system in which they orbit around their center of mass every 5. A study estimated the inclination is The orbital eccentricity is thought to be only 0. With a galactic latitude of 4 degrees and galactic longitude 71 degrees,  this system lies inward along the same Orion Spur in which the Sun is located within the Milky Way ,  near where the spur approaches the Sagittarius Arm.
From various techniques, the mass of the compact object appears to be greater than the maximum mass for a neutron star. Measuring periodicities in the X-ray emission near the object has yielded a more precise value of In all cases, the object is most likely a black hole   —a region of space with a gravitational field that is strong enough to prevent the escape of electromagnetic radiation from the interior.
Anything including matter and photons that passes through this boundary is unable to escape. Evidence of just such an event horizon may have been detected in using ultraviolet UV observations with the High Speed Photometer on the Hubble Space Telescope. As self-luminous clumps of matter spiral into a black hole, their radiation will be emitted in a series of pulses that are subject to gravitational redshift as the material approaches the horizon.
That is, the wavelengths of the radiation will steadily increase, as predicted by general relativity. Matter hitting a solid, compact object would emit a final burst of energy, whereas material passing through an event horizon would not. Two such "dying pulse trains" were observed, which is consistent with the existence of a black hole. The spin of the compact object is not yet well determined.
Given the current estimated mass of the black hole, the progenitor star must have lost over 30 solar masses of material. If the progenitor star had exploded as a supernova , then observations of similar objects show that the remnant would most likely have been ejected from the system at a relatively high velocity. As the object remained in orbit, this indicates that the progenitor may have collapsed directly into a black hole without exploding or at most produced only a relatively modest explosion.
The compact object is thought to be orbited by a thin, flat disk of accreting matter known as an accretion disk. This disk is intensely heated by friction between ionized gas in faster-moving inner orbits and that in slower outer ones. The mass of the compact object appears to determine the distance at which the surrounding plasma begins to emit these QPOs, with the emission radius decreasing as the mass decreases.
In the most common state, the X-rays are "hard", which means that more of the X-rays have high energy. In the less common state, the X-rays are "soft", with more of the X-rays having lower energy. The soft state also shows greater variability.
The hard state is believed to originate in a corona surrounding the inner part of the more opaque accretion disk. The spectral transition of Cygnus X-1 can be explained using a two component advective flow solution, as proposed by Chakrabarti and Titarchuk. As accreted matter falls toward the compact object, it loses gravitational potential energy. Part of this released energy is dissipated by jets of particles, aligned perpendicular to the accretion disk, that flow outward with relativistic velocities.
That is, the particles are moving at a significant fraction of the speed of light. This pair of jets provide a means for an accretion disk to shed excess energy and angular momentum. They may be created by magnetic fields within the gas that surrounds the compact object.
That is, they appear "dark". This collision appears to be forming a nebula that has been observed in the optical wavelengths. The signal was observed at the same time as a flare of hard X-rays, suggesting a link between the events. It has an estimated surface temperature of 31, K  and mass approximately 20—40 times the mass of the Sun. Based on a stellar evolutionary model, at the estimated distance of 2, parsecs this star may have a radius equal to about 15—17  times the solar radius and is approximately ,—, times the luminosity of the Sun.
This causes the optical brightness of the star to vary by 0.
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