A theory of photospheric emission from relativistic, collimated outflows
By C. Lundman, A. Pe’er, F. Ryde. 2012
149 citations recorded by the source corpus.
Relativistic outflows in the form of jets are common in many astrophysical objects. By their very nature, jets have angle-dependent velocity profiles, Γ=Γ(r, Θ, φ), where Γ is the outflow Lorentz factor. In this work we consider photospheric emission from non-dissipative jets with various Lorentz factor profiles, of the approximate form Γ ≈ Γ0/[(Θ/Θj)p + 1], where Θj is the characteristic jet opening angle. In collimated jets, the observed spectrum depends on the viewing angle, Θv. We show that for narrow jets (ΘjΓ0 l few), the obtained low-energy photon index is α ≈-1 (dN/dE / Eα), independent of viewing angle, and weakly dependent on the Lorentz factor gradient (p). A similar result is obtained for wider jets observed at Θv ≈ Θj. This result is surprisingly similar to the average low-energy photon index seen in gamma-ray bursts. For wide jets (ΘjΓ0 g few) observed at Θv g Θj, a multicolour blackbody spectrum is obtained. We discuss the consequences of this theory on our understanding of the prompt emission in gamma-ray bursts.
Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/e4d9b7655f1cf95fd1f7e79156bb02dcb97ee69d
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Citations in the corpus
- The physics of gamma-ray bursts & relativistic jets (2014, background): “And if the LF of the jet has an angular dependence such that it peaks at the jet axis and decreases with angle then the observed spectrum is flattened even further and can become fν ∝ ν0 (Lundman et al., 2013).”