Book contents
- Frontmatter
- Contents
- Index of Participants
- Preface
- I Evidence and Implications of Anisotropy in AGN
- II Luminosity Functions and Continuum Energy Distributions
- III The Broad Line Region: Variability and Structure
- IV X-rays and Accretion Disks
- V Beams, Jets and Blazars
- Magnetic Propulsion of Jets in AGN
- MHD Accretion-Ejection Model: X- and γ-rays and Formation of Relativistic Pair Beams
- Relativistic Electron Beams in AGN: Construction of Transonic Solutions
- Properties of Relativistic Jets
- A Massive Binary Black Hole in 1928+738?
- Gamma-Rays from Blazars: a Comparison of 3C 279, PKS 0537-441 and Mrk 421
- Microquasars in the Galactic Centre Region
- A Comparison of the Ultra-violet Continuum Variability Properties of Blazars and Seyfert 1s
- Simultaneous Optical and IR Monitoring of the Seyfert Nucleus NGC 7469
- Broad-Band Spectra and Polarization Properties of Variable Flat-Spectrum Radio Sources
- The Radio to Optical Variability of the BL Lac Object ON 231
- January 1992 Microvariability Campaign of OJ 287
- Blazar Microvariability: a Case Study of AO 0235+164
- Timescales of the Optical Variability of the BL Lacertae Galaxy PKS 2201+044
- Dynamics of Quasar Variability
- The Variability of a Large Sample of Quasars
- The Fate of Central Black Holes in Merging Galaxies
- Polarimetric Searching for Goldstone Bosons from AGNs
- VI Concluding Talk
Microquasars in the Galactic Centre Region
from V - Beams, Jets and Blazars
Published online by Cambridge University Press: 04 August 2010
- Frontmatter
- Contents
- Index of Participants
- Preface
- I Evidence and Implications of Anisotropy in AGN
- II Luminosity Functions and Continuum Energy Distributions
- III The Broad Line Region: Variability and Structure
- IV X-rays and Accretion Disks
- V Beams, Jets and Blazars
- Magnetic Propulsion of Jets in AGN
- MHD Accretion-Ejection Model: X- and γ-rays and Formation of Relativistic Pair Beams
- Relativistic Electron Beams in AGN: Construction of Transonic Solutions
- Properties of Relativistic Jets
- A Massive Binary Black Hole in 1928+738?
- Gamma-Rays from Blazars: a Comparison of 3C 279, PKS 0537-441 and Mrk 421
- Microquasars in the Galactic Centre Region
- A Comparison of the Ultra-violet Continuum Variability Properties of Blazars and Seyfert 1s
- Simultaneous Optical and IR Monitoring of the Seyfert Nucleus NGC 7469
- Broad-Band Spectra and Polarization Properties of Variable Flat-Spectrum Radio Sources
- The Radio to Optical Variability of the BL Lac Object ON 231
- January 1992 Microvariability Campaign of OJ 287
- Blazar Microvariability: a Case Study of AO 0235+164
- Timescales of the Optical Variability of the BL Lacertae Galaxy PKS 2201+044
- Dynamics of Quasar Variability
- The Variability of a Large Sample of Quasars
- The Fate of Central Black Holes in Merging Galaxies
- Polarimetric Searching for Goldstone Bosons from AGNs
- VI Concluding Talk
Summary
Abstract
The two persistent soft gamma-ray sources in the galactic centre region are black hole candidates of stellar mass with comptonized accretion disks that radiate 1037−38 erg s−1. They appear as microquasar stellar remnants from which emanate double-sided radio jets that extend over distances of a few parsecs.
The galactic centre in soft γ-rays
Contrary to the standard X-ray band (below 20keV), where many sources have been detected at less than 5° from the galactic centre, at higher energies (35-500 keV) the field is dominated by only two persistent sources: 1E1740.7-2942 and GRS1758-258 located respectively at ∼ 50′ and ∼ 5° from Sgr A (see Fig. 1). In the 30-500 keV band these sources radiate a few ×1037 erg s−1, near the Eddington limit of collapsed objects of stellar mass. Although persistent, they are time variable. Since no γ-ray source has been detected from Sgr A, if there is a super-massive black hole at the dynamic centre of the Galaxy, at present it is in sepulchral silence.
The telescope SIGMA on board GRANAT detected a powerful burst around 420 keV from the strongest γ-ray source 1E1740.7-2942 which is interpreted as the redshifted (probably gravitationally) 511 keV line from the annihilation of e+e− pairs. Since this Einstein source can produce and annihilate 10 billion (1010) tonnes of positrons in just one second, it is now known as the “Great Annihilator”. No annihilation line has yet been detected from GRS1758-258, the second strongest soft γ-ray source in that region.
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- The Nature of Compact Objects in Active Galactic NucleiProceedings of the 33rd Herstmonceux Conference, held in Cambridge, July 6-22, 1992, pp. 385 - 388Publisher: Cambridge University PressPrint publication year: 1994