FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W1992157598> ?p ?o ?g. }

• W1992157598 endingPage "1163" @default.
• W1992157598 startingPage "1151" @default.
• W1992157598 abstract "Particle acceleration in collisionless magnetic reconnection is studied in the relativistic regime of an electron-positron plasma. For the first time, the highly dynamic late-time evolution of reconnection is simulated in two dimensions (2D) and the finite size of the acceleration region is resolved in 3D applying a fully electromagnetic relativistic particle-in-cell (PIC) code. The late-time evolution is extremely important with respect to particle acceleration, because thin current sheets show a highly dynamic late-time phase with instabilities evolving in the Alfvén velocity vA0 regime. Consequently, since c∼vA0 is valid as a peculiarity of pair plasmas, v×B-contributions become dominant in the accelerating electric field. Most remarkable: Though acceleration regions are highly variable at late times, the power-law shape of the particle energy distribution is smoothed compared to quasi-static reconnection configurations at early times [S. Zenitani and M. Hoshino, Astrophys. J. 562, L63 (2001)]. Spectral power indices of s∼−3 for the complete simulation box, s∼−1 within the X-zone, are preserved at late times and appear as a characteristic of pair plasma reconnection of thin current sheets! The spectral high-energy cut-off depends on the sheet width at late times and is most efficiently tuned by the ratio c/vA0. In 3D, sheet instabilities limit the acceleration potential of a single X-zone, but current driven instabilities like the relativistic drift kink mode can also significantly contribute to particle acceleration. Via the analysis of particle trajectories, the consequences of a finite 3D acceleration zone are resolved and efficient acceleration mechanisms in the context of dynamic X-points are identified." @default.
• W1992157598 created "2016-06-24" @default.
• W1992157598 creator A5025606601 @default.
• W1992157598 creator A5030578797 @default.
• W1992157598 creator A5031102344 @default.
• W1992157598 creator A5087011620 @default.
• W1992157598 date "2004-02-19" @default.
• W1992157598 modified "2023-10-04" @default.
• W1992157598 title "Fast reconnection in relativistic pair plasmas: Analysis of particle acceleration in self-consistent full particle simulations" @default.
• W1992157598 cites W12802544 @default.
• W1992157598 cites W1507018549 @default.
• W1992157598 cites W1609343851 @default.
• W1992157598 cites W1970479591 @default.
• W1992157598 cites W1975502513 @default.
• W1992157598 cites W1978028455 @default.
• W1992157598 cites W1982012011 @default.
• W1992157598 cites W1983772292 @default.
• W1992157598 cites W2013862703 @default.
• W1992157598 cites W2021746310 @default.
• W1992157598 cites W2026768804 @default.
• W1992157598 cites W2028263180 @default.
• W1992157598 cites W2037305888 @default.
• W1992157598 cites W2040404323 @default.
• W1992157598 cites W2042306087 @default.
• W1992157598 cites W2048240043 @default.
• W1992157598 cites W2049413821 @default.
• W1992157598 cites W2053888331 @default.
• W1992157598 cites W2065556943 @default.
• W1992157598 cites W2072043284 @default.
• W1992157598 cites W2078719742 @default.
• W1992157598 cites W2082640301 @default.
• W1992157598 cites W2084911363 @default.
• W1992157598 cites W2087396768 @default.
• W1992157598 cites W2094017069 @default.
• W1992157598 cites W2094158461 @default.
• W1992157598 cites W2113872228 @default.
• W1992157598 cites W2153835871 @default.
• W1992157598 cites W2156430099 @default.
• W1992157598 cites W3098173778 @default.
• W1992157598 cites W3099817231 @default.
• W1992157598 cites W3105886888 @default.
• W1992157598 cites W3106164920 @default.
• W1992157598 doi "https://doi.org/10.1063/1.1644814" @default.
• W1992157598 hasPublicationYear "2004" @default.
• W1992157598 type Work @default.
• W1992157598 sameAs 1992157598 @default.
• W1992157598 citedByCount "112" @default.
• W1992157598 countsByYear W19921575982012 @default.
• W1992157598 countsByYear W19921575982013 @default.
• W1992157598 countsByYear W19921575982014 @default.
• W1992157598 countsByYear W19921575982015 @default.
• W1992157598 countsByYear W19921575982016 @default.
• W1992157598 countsByYear W19921575982017 @default.
• W1992157598 countsByYear W19921575982018 @default.
• W1992157598 countsByYear W19921575982019 @default.
• W1992157598 countsByYear W19921575982020 @default.
• W1992157598 countsByYear W19921575982021 @default.
• W1992157598 countsByYear W19921575982022 @default.
• W1992157598 countsByYear W19921575982023 @default.
• W1992157598 crossrefType "journal-article" @default.
• W1992157598 hasAuthorship W1992157598A5025606601 @default.
• W1992157598 hasAuthorship W1992157598A5030578797 @default.
• W1992157598 hasAuthorship W1992157598A5031102344 @default.
• W1992157598 hasAuthorship W1992157598A5087011620 @default.
• W1992157598 hasConcept C111368507 @default.
• W1992157598 hasConcept C117896860 @default.
• W1992157598 hasConcept C121332964 @default.
• W1992157598 hasConcept C127313418 @default.
• W1992157598 hasConcept C13966519 @default.
• W1992157598 hasConcept C147120987 @default.
• W1992157598 hasConcept C168997771 @default.
• W1992157598 hasConcept C2778517922 @default.
• W1992157598 hasConcept C30475298 @default.
• W1992157598 hasConcept C3079626 @default.
• W1992157598 hasConcept C31532427 @default.
• W1992157598 hasConcept C32127712 @default.
• W1992157598 hasConcept C36819163 @default.
• W1992157598 hasConcept C62520636 @default.
• W1992157598 hasConcept C74650414 @default.
• W1992157598 hasConcept C75183268 @default.
• W1992157598 hasConcept C82706917 @default.
• W1992157598 hasConcept C8426674 @default.
• W1992157598 hasConceptScore W1992157598C111368507 @default.
• W1992157598 hasConceptScore W1992157598C117896860 @default.
• W1992157598 hasConceptScore W1992157598C121332964 @default.
• W1992157598 hasConceptScore W1992157598C127313418 @default.
• W1992157598 hasConceptScore W1992157598C13966519 @default.
• W1992157598 hasConceptScore W1992157598C147120987 @default.
• W1992157598 hasConceptScore W1992157598C168997771 @default.
• W1992157598 hasConceptScore W1992157598C2778517922 @default.
• W1992157598 hasConceptScore W1992157598C30475298 @default.
• W1992157598 hasConceptScore W1992157598C3079626 @default.
• W1992157598 hasConceptScore W1992157598C31532427 @default.
• W1992157598 hasConceptScore W1992157598C32127712 @default.
• W1992157598 hasConceptScore W1992157598C36819163 @default.
• W1992157598 hasConceptScore W1992157598C62520636 @default.
• W1992157598 hasConceptScore W1992157598C74650414 @default.
• W1992157598 hasConceptScore W1992157598C75183268 @default.

• next