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Stability of non-neutral plasma in a magnetic dipole trap

ORAL

Abstract

A non-neutral plasma can be confined in a global thermal equilibrium state as well as a local

thermal equilibrium along magnetic field lines in a magnetic dipole trap [1]. While global ther-

mal equilibrium states are maximum entropy states and hence guaranteed to be stable, local

thermal equilibria can support growing diocotron modes [2]. These modes were studied to a

great extend in the homogeneous magnetic field of a Penning-Malmberg trap [3]. We will focus

on the inhomogeneous magnetic field of a z-pinch, which serves as an approximation of the

vicinity of a levitated coil. This implies two differences in comparison to a Penning-Malmberg

trap. First, grad-B and curvature drifts influence the mode. Second, arbitrary non-neutrality can be

studied. In particular, different fractions of electrons and positrons are considered. This study is

motivated by APEX, "A Positron-Electron eXperiment" in a levitated dipole trap [4].

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Publication: [1] Steinbrunner, P., et al., "Thermal Equilibrium of Collisional Non-Neutral Plasma in a Magnetic Dipole Trap"<br>Journal of Plasma Physics 89 (2023)<br>[2] Levy, Richard H. "Diocotron instability in a cylindrical geometry." The Physics of Fluids 8.7 (1965)<br>[3] Davidson, Ronald C. Physics of nonneutral plasmas. World Scientific Publishing Company, 2001.<br>[4] Stoneking, M. R., et al. "A new frontier in laboratory physics: magnetized electron–positron plasmas." Jour-<br>nal of Plasma Physics 86.6 (2020).

Presenters

  • Patrick Steinbrunner

    Max Planck Institute for Plasma Physics

Authors

  • Patrick Steinbrunner

    Max Planck Institute for Plasma Physics

  • Thomas M O'Neil

    University of California, San Diego