1993
DOI: 10.1103/physrevlett.71.2319
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Series of maxima in the field dependent magnetic moment of layered superconductors

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Cited by 103 publications
(77 citation statements)
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“…For example, for Yukawa particles the direct 2 − 3-transition was observed in dusty plasma clusters 24 with increasing linear density. In addition, a SOT has been predicted theoretically for an Abrikosovvortex arrangement in a superconducting slab for low temperatures [25][26][27][28][29] , for Pearl vortices 30 , and also for binary mixtures of repulsive particles 31 , in particular, when the ratio between charges of both species was around 1/5.…”
Section: Introductionmentioning
confidence: 99%
“…For example, for Yukawa particles the direct 2 − 3-transition was observed in dusty plasma clusters 24 with increasing linear density. In addition, a SOT has been predicted theoretically for an Abrikosovvortex arrangement in a superconducting slab for low temperatures [25][26][27][28][29] , for Pearl vortices 30 , and also for binary mixtures of repulsive particles 31 , in particular, when the ratio between charges of both species was around 1/5.…”
Section: Introductionmentioning
confidence: 99%
“…Such a "core explosion" transition of a vortex into a phase slip center can occur in thin films at temperatures T > T v because the coherence length ξ(T ) = ξ 0 (1 − T /T c ) −1/2 diverges at the critical temperature T c . The behavior of mesoscopic vortex structures in confined geometries has attracted much attention both experimentally 3 and theoretically 4,5 . Thermal fluctuations can radically change the behavior of vortices in thin films in a parallel field B.…”
mentioning
confidence: 99%
“…Note that as the film thickness increases the matching peaks become less evident in the magnetization loops, that is, the film gradually crosses over from mesoscopic to macroscopic behavior. The matching effect of vortex chains in thin slabs (W < λ) has been studied in the framework of thermodynamic equilibrium [13]. Our approach assumes that a vortex nucleates at the surfaces, i.e., for fields just above H c1 it has to overcome a strong energy barrier in order to find the global minimum at the equatorial plane of the film.…”
Section: Vortex Chain States In Mesoscopic Filmsmentioning
confidence: 99%