Abstract

Gamma-ray bursts (GRBs) are brief but intense emission of soft γ\gamma-rays, mostly lasting from a few seconds to a few thousand seconds. For such kind of high energy transients, their isotropic-equivalent-energy (EisoE_{\rm iso}) function may be more scientifically meaningful when compared with GRB isotropic-equivalent-luminosity function (LisoL_{\rm iso}), as the traditional luminosity function refers to steady emission much longer than a few thousand seconds. In this work we for the first time construct the isotropic-equivalent-energy function for a sample of 95 bursts with measured redshifts (zz) and find an excess of high-zz GRBs. Assuming that the excess is caused by a GRB luminosity function evolution in a power-law form, we find a cosmic evolution of Eiso(1+z)1.800.63+0.36E_{\rm iso}\propto(1+z)^{1.80^{+0.36}_{-0.63}}, which is comparable to that between LisoL_{\rm iso} and zz, i.e., Liso(1+z)2.300.51+0.56L_{\rm iso}\propto(1+z)^{2.30^{+0.56}_{-0.51}} (both 1σ1\sigma). The evolution-removed isotropic-equivalent-energy function can be reasonably fitted by a broken power-law, in which the dim and bright segments are ψ(Eiso)Eiso0.27±0.01\psi(E_{\rm iso})\propto E_{\rm iso}^{-0.27\pm0.01} and ψ(Eiso)Eiso0.87±0.07\psi(E_{\rm iso})\propto E_{\rm iso}^{-0.87\pm0.07}, respectively (1σ1\sigma). For the cosmic GRB formation rate, it increases quickly in the region of 0z10 \leq z \lesssim 1, and roughly keeps constant for 1z41\lesssim z \lesssim 4, and finally falls with a power index of 3.80±2.16-3.80\pm2.16 for z4z\gtrsim 4, in good agreement with the observed cosmic star formation rate so far.Comment: 6 pages, 10 figures. Accepted for publication in MNRA

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