2005
DOI: 10.1007/bf02769584
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Flux-line cutting in hard superconductors

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Cited by 3 publications
(7 citation statements)
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“…In addition, in the geometry of crossed fields, the OECSM is able to reproduce the families of experimental curves [30,31] of the average magnetization for a VTi ribbon versus the external magnetic field H y for the components M y and M z at different dc-bias fields H z and for initial nonmagnetic states. The good agreement between theory [27,29] and experiments [30,31] was achieved using a large anisotropy parameter J c /J c⊥ = 6.…”
Section: Introductionsupporting
confidence: 58%
See 1 more Smart Citation
“…In addition, in the geometry of crossed fields, the OECSM is able to reproduce the families of experimental curves [30,31] of the average magnetization for a VTi ribbon versus the external magnetic field H y for the components M y and M z at different dc-bias fields H z and for initial nonmagnetic states. The good agreement between theory [27,29] and experiments [30,31] was achieved using a large anisotropy parameter J c /J c⊥ = 6.…”
Section: Introductionsupporting
confidence: 58%
“…For this reason, new models have been proposed to explain both the collapse of the magnetic moment and the phenomena arising when the anisotropy induced by flux-line cutting is considerably high. Among them, we should mention (i) the extension to the GDCSM model (hereafter the BMM), proposed by Brandt and Mikitik [25]; (ii) the variational approach developed by Badía-Majós, López, and Ruiz (here called BLRM) [26]; and (iii) the original elliptic flux-cutting critical-state model (OECSM) [27][28][29]. The latter model postulates…”
Section: Introductionmentioning
confidence: 99%
“…[23,24]. The elliptic model also describes the behavior of < M y > (H y ) and < M z > (H y ) in crossed fields H y and H z [19,25], which was observed in the experiments on a VTi ribbon with nonmagnetic initial state [14,26]. Here, the good agreement with the experiment was achieved by using a relatively large anisotropy parameter J c /J c⊥ = 6.…”
Section: Introductionmentioning
confidence: 62%
“…21 Due to the limitations of the GDCSM and the TVHM, the elliptic flux-line-cutting critical-state model ͑EFLCCSM͒ 3 was introduced. This simple phenomenological model had described quite well the magnetic response of slabs, in parallel geometry, for multicomponent situations, 3,26,27 in comparison with previous models. According to the EFLCCSM material law E͑J͒, each component J Ќ and J ʈ of the current density is determined by both components of the electric field E Ќ and E ʈ .…”
Section: Introductionmentioning
confidence: 85%
“…Thus, at present, the flux-line-cutting phenomenon is an interesting topic of research. 3,5,10,11,[13][14][15][16][17][18][19][20][21][22][23][24][25][26][27] Indeed, there is experimental evidence, related with the crossing energy calculation, which supports that a small number of vortices or adjacent sheets of vortices can cut through each other. [28][29][30][31][32] Recently, Olson Reichhardt and Hastings have proposed an experiment employing a magnetic force microscope to test how easily the vortex lines can cut through each other.…”
Section: Introductionmentioning
confidence: 97%