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Equatorial outflows driven by jets in Population III microquasars

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Abstract

Binary systems of Population III can evolve to microquasars when one of the stars collapses into a black hole. When the compact object accretes matter at a rate greater than the Eddington rate, powerful jets and winds driven by strong radiation pressure should form. We investigate the structure of the jet-wind system for a model of Population III microquasar on scales beyond the jet-wind formation region. Using relativistic hydrodynamic simulations we find that the ratio of kinetic power between the jet and the disk wind determines the configuration of the system. When the power is dominated by the wind, the jet fills a narrow channel, collimated by the dense outflow. When the jet dominates the power of the system, part of its energy is diverted turning the wind into a quasi-equatorial flow, while the jet widens. From the results of our simulations, we implement semi-analytical calculations of the impact of the quasi-equatorial wind on scales of the order of the size of the binary system. Our results indicate that Population III microquasars might inject gamma rays and relativistic particles into the early intergalactic medium, contributing to its reionization at large distances from the binary system.

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Notes

  1. In the super-critical accretion regime, there exists some critical radius \(r_{\mathrm{cr}}\) such that outside \(r_{\mathrm{cr}}\), the accretion rate is constant and the disk is a radiation-pressure dominated standard disk. Inside \(r_{\mathrm{cr}}\), the accretion rate decreases with the radius as to maintain the critical rate, expelling the excess of mass by the radiation-driven wind (Fukue 2004).

  2. One can still assume that some fraction of the jet energy can be in the form of radiating non-thermal particles, but we assume that such a component will not affect the jet dynamics.

  3. The equatorial wind in Population III microquasars does not stop accretion. In these systems the accretion is by overflowing the Roche lobe, therefore the accreted matter flows only in the plane where the Lagrange point is contained, while the equatorial wind is always directed above the accretion disk. On the contrary, accretion arrest could occur if mass transfer from the star is by stellar winds, as in Population I microquasars.

  4. The particle acceleration rate depends on the shock velocity and the diffusion coefficient of the medium. For both shocks parallel or perpendicular to the magnetic field, the diffusion coefficient is a multiple of the Bohm diffusion coefficient, therefore the acceleration timescale is inversely proportional to the gyroradius of the particles (See Drury 1983).

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Acknowledgements

PSC is Fellow of CONICET and PhD student at Universidad Nacional de La Plata (UNLP). PSC thanks the UNLP for the training received during his undergraduate studies, and the public education system in Argentina. GER is very grateful to the ICCUB where part of this research was done. This work was supported by the Argentine agency CONICET (PIP 2014-00338) and the Spanish Ministerio de Ciencia e Innovación (MICINN) under grant PID2019-105510GBC31 and though the “Center of Excellence María de Maeztu 2020-2023” award to the ICCUB (CEX2019-000918-M). V.B-R. is Correspondent Researcher of CONICET, Argentina, at the IAR.

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Correspondence to Pablo Sotomayor Checa.

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Sotomayor Checa, P., Romero, G.E. & Bosch-Ramon, V. Equatorial outflows driven by jets in Population III microquasars. Astrophys Space Sci 366, 13 (2021). https://doi.org/10.1007/s10509-020-03911-5

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