Compressive Structures in the Foreshock of Collisionless Shocks

dc.contributor.authorRaptis, Savvas
dc.contributor.authorTrotta, Domenico
dc.contributor.authorTurner, Drew L.
dc.contributor.authorBlanco-Cano, Xóchitl
dc.contributor.authorHietala, Heli
dc.contributor.authorKarlsson, Tomas
dc.contributor.authorJebaraj, Immanuel Christopher
dc.contributor.authorVasko, Ivan Y.
dc.contributor.authorOsmane, Adnane
dc.contributor.authorTakahashi, Kazue
dc.contributor.authorLario, David
dc.contributor.authorWilson, Lynn B.
dc.contributor.authorHowes, Gregory G.
dc.contributor.authorWimmer-Schweingruber, Robert F.
dc.contributor.organizationfi=avaruustutkimuslaboratorio|en=Space Research Laboratory|
dc.contributor.organization-code1.2.246.10.2458963.20.47833719389
dc.converis.publication-id523364103
dc.converis.urlhttps://research.utu.fi/converis/portal/Publication/523364103
dc.date.accessioned2026-05-15T20:11:50Z
dc.description.abstract<p>Collisionless shocks are fundamental accelerators of energetic particles, yet the observations of nonlinear foreshock structures, which are essential in acceleration processes, differ significantly between interplanetary (IP) shocks and planetary bow shocks. We present a direct comparison of two high-Mach-number, quasi-parallel shocks: an IP shock observed by Solar Orbiter and the Earth’s bow shock measured by the Magnetospheric Multiscale mission during the 2024–2025 “string-of-pearls” campaign. We show that foreshock compressive structures (FCSs) initiate upstream of both shocks at similar normalized distances (≲50 ion inertial lengths, <em>d</em><sub><em>i</em></sub>) when the suprathermal (>10 keV) ion density exceeds ∼1% of the background. However, the IP shock lacks the fully evolved, high-amplitude short large-amplitude magnetic structures characteristic of the terrestrial foreshock. We demonstrate that the “growth zone” capable of sustaining these structures is spatially limited (∼135 <em>d</em><sub><em>i</em></sub>), which, due to the high speed of the propagating IP shock, corresponds to a brief observational window of <10 s. Beyond this observational constraint, we suggest an additional physical mechanism that can inhibit foreshock maturity at IP shocks. The lack of global curvature prevents the lateral supply (“cross talk”) of energetic ions from different shock regions. These findings suggest that while the fundamental physics of FCS initiation is unified across collisionless shocks, the achievement of full nonlinearity can be regulated by the unique shock geometry and upstream properties while ultimately remaining observationally challenging to identify.</p>
dc.identifier.eissn2041-8213
dc.identifier.jour-issn2041-8205
dc.identifier.urihttps://www.utupub.fi/handle/11111/60721
dc.identifier.urlhttps://doi.org/10.3847/2041-8213/ae53e5
dc.identifier.urnURN:NBN:fi-fe2026051546207
dc.language.isoen
dc.okm.affiliatedauthorJeba Raj, Immanuel
dc.okm.discipline115 Astronomy and space scienceen_GB
dc.okm.discipline115 Avaruustieteet ja tähtitiedefi_FI
dc.okm.discipline114 Physical sciencesen_GB
dc.okm.discipline114 Fysiikkafi_FI
dc.okm.internationalcopublicationinternational co-publication
dc.okm.internationalityInternational publication
dc.okm.typeA1 ScientificArticle
dc.publisherInstitute of Physics Publishing
dc.publisher.countryUnited Kingdomen_GB
dc.publisher.countryBritanniafi_FI
dc.publisher.country-codeGB
dc.relation.articlenumberL55
dc.relation.doi10.3847/2041-8213/ae53e5
dc.relation.ispartofjournalAstrophysical Journal Letters
dc.relation.issue2
dc.relation.volume1000
dc.titleCompressive Structures in the Foreshock of Collisionless Shocks
dc.year.issued2026

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