Observations of pressure anisotropy effects within semi-collisional magnetized plasma bubbles.
Nat Commun 2021;
12:334. [PMID:
33436570 PMCID:
PMC8115095 DOI:
10.1038/s41467-020-20387-7]
[Citation(s) in RCA: 9] [Impact Index Per Article: 2.3] [Reference Citation Analysis] [Abstract] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 03/06/2020] [Accepted: 11/24/2020] [Indexed: 11/09/2022] Open
Abstract
Magnetized plasma interactions are ubiquitous in astrophysical and
laboratory plasmas. Various physical effects have been shown to be important within
colliding plasma flows influenced by opposing magnetic fields, however, experimental
verification of the mechanisms within the interaction region has remained elusive.
Here we discuss a laser-plasma experiment whereby experimental results verify that
Biermann battery generated magnetic fields are advected by Nernst flows and
anisotropic pressure effects dominate these flows in a reconnection region. These
fields are mapped using time-resolved proton probing in multiple directions. Various
experimental, modelling and analytical techniques demonstrate the importance of
anisotropic pressure in semi-collisional, high-β
plasmas, causing a reduction in the magnitude of the reconnecting fields when
compared to resistive processes. Anisotropic pressure dynamics are crucial in
collisionless plasmas, but are often neglected in collisional plasmas. We show
pressure anisotropy to be essential in maintaining the interaction layer,
redistributing magnetic fields even for semi-collisional, high energy density
physics (HEDP) regimes.
Magnetic fields can be reorganized by plasma flows and lead to effects
such as magnetic reconnection. Here the authors explore the evolution of
magnetized-plasma bubbles in a semi-collisional regime and the role of pressure
anisotropy in influencing the flow of the laser-produced plasma.
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