Gamma‐ray burst distance scales are reviewed. Most observations are inconsistent with metagalactic (D≳30 Mpc) or extragalactic (100 Kpc <D<30 Mpc) distances. For Galactic distances (D<100 Kpc) disks or a conventional halo are improbable. The possibility that bursts occupy the Galaxy’s massive extended halo (MEH) is examined. Such distributions provide the best fit to the data. MEH bursts are characterized by a maximum burst luminosity L2(≳30 keV)≤1042 ergs, an intrinsic luminosity distribution peaked toward low luminosity and having a range of ∼100, and a Galactic center burst rate density n0(0)∼1011 pc−3‐yr−1. The total Galactic burst rate is ∼400 yr−1 and the nearest burst source should lie between 5 and 1.4 Kpc for burst repetitions of 1 to 50 yrs. The high burst luminosity suggests bursts in M31 may be visible near current thresholds, i.e., ∼185 yr−1 with S≳10−8 ergs‐cm−2. A 3σ detection of M31 should be possible with one year of observation using a threshold of 10−7 ergs‐cm−2.
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26 May 1984
High Energy Transients in Astrophysics
11-22 July 1983
Santa Cruz, CA, USA
Research Article|
May 26 1984
The gamma‐ray burst spatial distribution logN(≳S) vs logs and N(≳S,1II,bII) vs s
Mark C. Jennings
Mark C. Jennings
Institute of Geophysics and Planetary Physics University of California, Riverside, CA 92521
Los Alamos National Laboratory Los Alamos, NM 87544
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AIP Conf. Proc. 115, 412–421 (1984)
Citation
Mark C. Jennings; The gamma‐ray burst spatial distribution logN(≳S) vs logs and N(≳S,1II,bII) vs s. AIP Conf. Proc. 26 May 1984; 115 (1): 412–421. https://doi.org/10.1063/1.34550
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