Abstract

We describe here efforts to create and study magnetized electron–positron pair plasmas, the existence of which in astrophysical environments is well-established. Laboratory incarnations of such systems are becoming ever more possible due to novel approaches and techniques in plasma, beam and laser physics. Traditional magnetized plasmas studied to date, both in nature and in the laboratory, exhibit a host of different wave types, many of which are generically unstable and evolve into turbulence or violent instabilities. This complexity and the instability of these waves stem to a large degree from the difference in mass between the positively and the negatively charged species: the ions and the electrons. The mass symmetry of pair plasmas, on the other hand, results in unique behaviour, a topic that has been intensively studied theoretically and numerically for decades, but experimental studies are still in the early stages of development. A levitated dipole device is now under construction to study magnetized low-energy, short-Debye-length electron–positron plasmas; this experiment, as well as a stellarator device that is in the planning stage, will be fuelled by a reactor-based positron source and make use of state-of-the-art positron cooling and storage techniques. Relativistic pair plasmas with very different parameters will be created using pair production resulting from intense laser–matter interactions and will be confined in a high-field mirror configuration. We highlight the differences between and similarities among these approaches, and discuss the unique physics insights that can be gained by these studies.

Highlights

  • Plasma physics has had tremendous success in developing our understanding of the most observable state of matter in the universe, and today it is at the heart of diverse scientific and industrial applications

  • It was recognized more than 40 years ago that the physics of pair plasmas is truly unique (Tsytovich & Wharton 1978), and around the same time it was proposed that magnetized electron–positron plasmas likely exist around pulsars (Arons 1979)

  • Theoretical work aimed at explaining intense non-thermal radiation from astrophysical phenomena such as gamma-ray bursts (GRB) has focused on particle acceleration in collisionless shocks formed through Weibel-like instabilities (Weibel 1959) in relativistic electron–positron plasma (Yang et al 1993)

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Summary

Introduction

Plasma physics has had tremendous success in developing our understanding of the most observable state of matter in the universe, and today it is at the heart of diverse scientific and industrial applications. That for the same reasons that the ion acoustic wave is suppressed in a pair plasma because the equal masses of the positive and negative charged particles eliminates the electric field that sustains it; drift waves and their associated instabilities should be largely absent in such systems possessing a confining magnetic field. Since the Debye length scales as the inverse square root of the density, whereas the Larmor radius (which is the step size for collisional transport in the usual regime) is independent of density, the classical Coulomb transport associated with low density pair plasmas could be the dominant transport mechanism If this is verified experimentally, it would be the first time that a magnetically confined quasi-neutral plasma is free of anomalous transport. Nor can we reliably predict the nonlinear saturation of these instabilities

Instabilities in relativistic pair plasma
Timeliness of electron–positron plasma studies
Levitated dipole and stellarator
Target parameters for magnetically confined pair plasma experiments
Annihilation of positrons does not rule out long confinement
The importance of a small Debye length
Plans for the APEX levitated dipole and the EPOS optimized stellarator
The importance of the plasma skin depth
Parameters for laser-produced pairs
Magnetic confinement of laser-produced pairs
Summary

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