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dc.contributor.authorLevesque, Joseph M.en_US
dc.contributor.authorLiao, Andy S.en_US
dc.contributor.authorHartigan, Patricken_US
dc.contributor.authorYoung, Rachel P.en_US
dc.contributor.authorTrantham, Matthewsen_US
dc.contributor.authorGray, Williamsen_US
dc.contributor.authorKlein, Salleeen_US
dc.contributor.authorManuel, Marioen_US
dc.contributor.authorFiksel, Gennadyen_US
dc.contributor.authorKatz, Josephen_US
dc.contributor.authorLi, Chi-Kangen_US
dc.contributor.authorBirkel, Andrewen_US
dc.contributor.authorTzeferacos, Petrosen_US
dc.contributor.authorKuranz, Carolyn C.en_US
dc.date.accessioned2025-03-21T20:16:48Z
dc.date.available2025-03-21T20:16:48Z
dc.date.issued2021-07
dc.identifier21ja034
dc.identifier.urihttps://hdl.handle.net/1721.1/158641
dc.descriptionSubmitted for publication in Physics of Plasmas
dc.description.abstractThe magnetic field produced by planets with active dynamos, like the Earth, can exert sufficient pressure to oppose supersonic stellar wind plasmas, leading to the formation of a standing bow shock upstream of the magnetopause, or pressure-balance surface. Scaled laboratory experiments studying the interaction of an inflowing solar wind analog with a strong, external magnetic field are a promising new way to study magnetospheric physics and to complement existing models, although reaching regimes favorable for magnetized shock formation is experimentally challenging. This paper presents experimental evidence of the formation of a magnetized bow shock in the interaction of a supersonic, super-Alfvenic plasma with a strongly magnetized obstacle at the OMEGA laser facility. The solar wind analog is generated by the collision and subsequent expansion of two counter- propagating, laser-driven plasma plumes. The magnetized obstacle is a thin wire, driven with strong electrical currents. Hydrodynamic simulations using the FLASH code predict that the colliding plasma source meets the criteria for bow shock formation. Spatially resolved, optical Thomson scat- tering measures the electron number density, and optical emission lines provide a measurement of the plasma temperature, from which we infer the presence of a fast magnetosonic shock far upstream of the obstacle. Proton images provide a measure of large-scale features in the magnetic field topology, and reconstructed path-integrated magnetic field maps from these images suggest the formation of a bow shock upstream of the wire and as a transient magnetopause. We compare features in the reconstructed fields to two-dimensional MHD simulations of the system.
dc.publisherAIPen_US
dc.relation.isversionofdoi.org/10.1063/5.0062254
dc.sourcePlasma Science and Fusion Centeren_US
dc.titleExperimental observations of detached bow shock formation in the interaction of a laser-produced plasma with a magnetized obstacleen_US
dc.typeArticleen_US
dc.contributor.departmentMassachusetts Institute of Technology. Plasma Science and Fusion Center
dc.relation.journalPhysics of Plasmas


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