The luminosity function and the rate of Swift's Gamma Ray Bursts
By D. Wanderman, T. Piran. 2009
283 citations recorded by the source corpus.
We invert directly the redshift-luminosity distribution of observed long Swift gamma-ray bursts (GRBs) to obtain their rate and luminosity function. Our best-fitting rate is described by a broken power law that rises like (1 + 2) 2.1+0.5 -0.6 for 0 3. The local rate is ρ 0 ≃ 1.3 +0.6 -0.7 (Gpc -3 yr -1 ). The luminosity function is well described by a broken power law with a break at L* ≃ 10 52.5±0.2 (erg s -1 ) and with indices α = 0.2 +0.2 -0.1 and β = 1.4 +0.3 -0.6 . The recently detected GRB 090423, with z ≈ 8, fits nicely into the model's prediction, verifying that we are allowed to extend our results to high redshifts. While the GRB rate may follow the star formation rate (SFR) for z < 3, the high-redshift slope is shallower than the steep decline in the SFR for 4 < z. However, we cannot rule out a GRB rate that follows one of the recent SFR models.
Subfields: Astronomy and Astrophysics
View Paper: https://www.semanticscholar.org/paper/1b6a979f335598c379f5c2b30458bec10b464a41
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In Astronomy and Astrophysics
Citations in the corpus
- CONNECTING THE GAMMA RAY BURST RATE AND THE COSMIC STAR FORMATION HISTORY: IMPLICATIONS FOR REIONIZATION AND GALAXY EVOLUTION (2011, background): “In other words, the decline in the GRB rate at z > 4 is considerably less rapid than the decrease in the star formation rate (e.g., Wanderman & Piran 2010).”
- THE OBSERVABLE SIGNATURES OF GRB COCOONS (2016, methodology): “We take RGRBs ≈ 1Gpc−3yr−1 as the local rate of observed LGRBs, i.e., GRBs with jet that points towards us (e.g., Wanderman & Piran 2010).”
- The Zwicky Transient Facility Bright Transient Survey. II. A Public Statistical Sample for Exploring Supernova Demographics (2020, methodology): “The GRB rate is consistent with expectations given the on-axis GRB rate of ∼1 Gpc−3 yr−1 (Wanderman & Piran 2010), assuming we would only be sensitive to events seen within a viewing angle of θ<3θjet at this luminosity threshold.”
- Millisecond Magnetar Birth Connects FRB 121102 to Superluminous Supernovae and Long-duration Gamma-Ray Bursts (2017, methodology): “This is comparable to the estimated beaming-correct local (z ≈ 0) rate of LGRBs of ≈ 130+60−70 Gpc−3 yr−1 for an assumed beaming fraction of fb = 1/100 (Wanderman & Piran 2010).”
- The physics of gamma-ray bursts & relativistic jets (2014, background): “Several studies agree that the high-luminosity slope is steep: α2 ∼ 2.5 (e.g. Liang et al., 2007a; Virgili et al., 2009; Wanderman and Piran, 2010).”
- The rate, luminosity function and time delay of non-Collapsar short GRBs (2014, methodology): “When comparing the luminosity function found here for sGRBs with the long GRBs luminosity function (Wanderman & Piran 2010) we find that the break luminosity is close (L∗sGRB = 2 × 1052 and L∗LGRB = 3 × 1052), but the sGRB luminosity function is steeper compared with the LGRB luminosity function…”
- Stellar black holes at the dawn of the universe (2011, background): “There is increasing evidence for an enhanced LGRB rate at z > 3 (Daigne et al. 2006; Kistler et al. 2008; Wanderman & Piran 2010; Qin et al. 2010), as expected from the increase in the specific star formation rate (SFR) with decreasing metallicity (Mannucci et al. 2010).”