2002
DOI: 10.1103/physrevb.66.014509
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Phase transitions in isolated vortex chains

Abstract: In very anisotropic layered superconductors (e.g. Bi2Sr2CaCu2Ox) a tilted magnetic field can penetrate as two co-existing lattices of vortices parallel and perpendicular to the layers. At low out-of-plane fields the perpendicular vortices form a set of isolated vortex chains, which have recently been observed in detail with scanning Hall-probe measurements. We present calculations that show a very delicate stability of this isolated-chain state. As the vortex density increases along the chain there is a first-… Show more

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Cited by 35 publications
(14 citation statements)
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“…The discussed structure of a PV line crossed by a JV stack has a pronounced effect on vortex interactions [28] in crossing-lattice states of layered superconductors as well as their magnetization. For example, the tilt produces a dipole moment for all PV lines (even in the Abrikosov regions in between JV stacks), which generates an attraction between PV stacks [29].…”
mentioning
confidence: 98%
“…The discussed structure of a PV line crossed by a JV stack has a pronounced effect on vortex interactions [28] in crossing-lattice states of layered superconductors as well as their magnetization. For example, the tilt produces a dipole moment for all PV lines (even in the Abrikosov regions in between JV stacks), which generates an attraction between PV stacks [29].…”
mentioning
confidence: 98%
“…Condensates can afford a rich variety of vortex-cluster structures, including soliton-vortex hybrids 29 , vortex chains 39 40 , turbulent vortex tangles 41 , corotating vortices 42 vortex dipoles 13 43 44 45 46 47 48 , vortex tripoles 49 50 and vortex quadrupoles 51 52 53 54 55 . Different from the vortex lattice induced by the rotation of BECs 56 57 58 59 , the complex structures made by vortices with opposite charges are excited collective states of nonrotating BECs.…”
mentioning
confidence: 99%
“…19,20 At very small c-axis fields (∼ several gauss) the regions of triangular lattice vanish leaving only chains of stacks. 17 Moreover, there are experimental indications 17 and theoretical reasoning 21 in favor of the phase transition from the crossing configuration of pancake-stack chains and JVs into chains of tilted vortices. JVs also modify the interaction between pancake stacks leading to an attractive interaction between the stacks at large distances.…”
Section: Introductionmentioning
confidence: 99%