Abstract

Context. The origin of Galactic cosmic rays remains a matter of debate, but supernova remnants are commonly considered to be the main place where high-energy cosmic rays are accelerated. Nevertheless, current models predict cosmic-ray spectra that do not match observations and the efficiency of the acceleration mechanism is still undetermined. On the other hand, the contribution of other kinds of sources to the Galactic cosmic-ray population is still unclear, and merits investigation. Aims. In this work we explore a novel mechanism through which microquasars might produce cosmic rays. In this scenario, microquasar jets generate relativistic neutrons, which escape and decay outside the system; protons and electrons, created when these neutrons decay, escape to the interstellar medium as cosmic rays. Methods. We introduce the relativistic neutron component through a coupling term in the transport equation that governs the jet proton population. We compute the escape rate and decay distribution of these neutrons, and follow the propagation of the decay products until they escape the system and become cosmic rays. We then compute the spectra of these cosmic rays. Results. Neutrons can drain only a small fraction of the jet power as cosmic rays. The most promising scenarios arise in extremely luminous systems (Ljet ∼ 1040 erg s−1), in which the fraction of jet power deposited in cosmic rays can reach ∼0.001. Slow jets (Γ ≲ 2, where Γ is the bulk Lorentz factor) favour neutron production. The resulting cosmic-ray spectrum is similar for protons and electrons, which share the power in the ratio given by neutron decay. The spectrum peaks at roughly half the minimum energy of the relativistic protons in the jet; it is soft (spectral index ∼3) above this energy, and almost flat below. Conclusions. The proposed mechanism produces more energetic cosmic rays from microquasars than those presented by previous works in which the particles escape through the jet terminal shock. Values of spectral index steeper than 2 are possible for cosmic rays in our model and these indeed agree with those required to explain the spectral signatures of Galactic cosmic rays, although only the most extreme microquasars provide power comparable to that of a typical supernova remnant. The mechanism explored in this work may provide stronger and softer cosmic-ray sources in the early Universe, and therefore contribute to the heating and reionisation of the intergalactic medium.

Highlights

  • Microquasars (MQs) are X-ray binaries (XRBs) with relativistic jets

  • In which cosmic rays (CRs) are produced at the terminal shock of the jet, we propose that CRs may be injected directly into the interstellar medium (ISM) by relativistic neutrons escaping from the jet

  • We introduced the relativistic neutron component in hadronic jet models through inelastic proton-proton collisions that produce these particles in situ

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Summary

Introduction

Microquasars (MQs) are X-ray binaries (XRBs) with relativistic jets. These systems display a phenomenology that resembles that of active galactic nuclei (AGNs) but on smaller scales (Mirabel & Rodríguez 1994). Likewise, Heinz & Sunyaev (2002) model a mechanism in which a narrow band of the CR spectrum is produced in the terminal shocks of MQ jets This sharp spectrum has a characteristic proton energy that depends on the bulk Lorentz factor of the jet. In which CRs are produced at the terminal shock of the jet, we propose that CRs may be injected directly into the ISM by relativistic neutrons escaping from the jet. These neutrons are produced by the interaction of protons accelerated in internal shocks with thermal ones. Injection of protons in the acceleration region is described by a source rate density

Jet model
The jet of Cygnus X-1
Stellar wind contribution
Other jet scenarios
Neutron decay
Cosmic-ray spectra
Findings
Discussion and conclusions
Full Text
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