2004
DOI: 10.12693/aphyspola.106.693
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Superconducting Pinning by Magnetic Domains in a Ferromagnet-Superconductor Bilayer

Abstract: The local flux profile and the critical current are studied using an array of Hall sensors in a ferromagnetic-superconducting bilayer which consists of niobium film covering ferromagnetic Co/Pt multilayer with perpendicular magnetic anisotropy. The results indicate about threefold enhancement of the flux pinning in niobium layer caused by the isolated magnetic domains which are created during the magnetization reversal of the Co/Pt multilayer. The geometrical barrier is absent, and the critical current is stro… Show more

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Cited by 4 publications
(7 citation statements)
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“…The deviation of s from 1 or 0 leads to a strong asymmetry of the loops with respect to the direction of H, indicating the enhancement of vortex pinning when H is positive. This is a result of the magnetic pinning induced by the presence of positive residual magnetic domains, similar to the one described previously in Nb5 sample [4][5][6]. The magnitude of the pinning enhancement is larger in Nb8 sample by a factor of about 1.5, which may be attributed to a larger magnetic moment resulting from the larger amount of Co/Pt repeats.…”
Section: Magnetic Pinningsupporting
confidence: 82%
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“…The deviation of s from 1 or 0 leads to a strong asymmetry of the loops with respect to the direction of H, indicating the enhancement of vortex pinning when H is positive. This is a result of the magnetic pinning induced by the presence of positive residual magnetic domains, similar to the one described previously in Nb5 sample [4][5][6]. The magnitude of the pinning enhancement is larger in Nb8 sample by a factor of about 1.5, which may be attributed to a larger magnetic moment resulting from the larger amount of Co/Pt repeats.…”
Section: Magnetic Pinningsupporting
confidence: 82%
“…The loop is typical of samples with perpendicular magnetic anisotropy, with rapid decrease in magnetic moment in the first stage of the MRP, followed by a slower decrease (tail) in the second stage when the remaining uninverted domains are gradually removed by increasing magnetic field. The loop for Nb5 sample is similar, as described previously [4][5][6], except for coercive fields which are 610 Oe and 700 Oe for the samples Nb5 and Nb8, respectively. The magnetic force microscope (MFM) imaging in the remnant state at 300 K shows that the MRP in Nb8 sample starts from several nucleation centers, from which a fractal structure of inverted domains gradually grows to cover the whole sample.…”
Section: Samplesmentioning
confidence: 89%
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“…The domain structure in FSB's may be reversibly defined and erased allowing easy modulation of pinning. While there are many experiments which confirm the existence of the MP, only few of them attempt to correlate the vortex dynamics in the FSB's with the geometry of the magnetic domain patterns [3][4][5][6][7][8][9][10].…”
Section: Introductionmentioning
confidence: 99%