2014
DOI: 10.1016/j.physc.2014.06.017
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Dynamics of vortex matter in YBCO sub-micron bridges

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Cited by 21 publications
(15 citation statements)
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“…Both the magnetoresistance and temperature, R(T ), dependences, are taken employing a lock-in amplifier, feeding the sample with a current modulated at 17.3 Hz. Excitation signals were of the order of 300 nA to avoid heating and/or excessive perturbation of vortex dynamics27 effects. Magnetic field step was about Δ B  = 10 mT, i.e., one tenth of the expected B c1 (see below).…”
Section: Methodsmentioning
confidence: 99%
“…Both the magnetoresistance and temperature, R(T ), dependences, are taken employing a lock-in amplifier, feeding the sample with a current modulated at 17.3 Hz. Excitation signals were of the order of 300 nA to avoid heating and/or excessive perturbation of vortex dynamics27 effects. Magnetic field step was about Δ B  = 10 mT, i.e., one tenth of the expected B c1 (see below).…”
Section: Methodsmentioning
confidence: 99%
“…The curves are characterized by a broadening, which is larger in 3EBL devices. Such a broadening, expected in nanowires with width w much larger than the coherence length ξ [w ≫ 4.4ξðTÞ even at T ≈ T C ], can be ascribed to the dissipation induced by vortices, perpendicular to the bias current, crossing the nanowire [35][36][37][38]. The resistance of 1EBL and 3EBL nanowires can be written as…”
Section: B Analysis Of the Resistance Versus Temperature Transitionmentioning
confidence: 99%
“…In 2D wires like the one of Figs. 3-5, where the width is much bigger than the coherence length ξ(w 4.4ξ(T )) even at T ≈ T C , vortices crossing the wire, perpendicular to the bias current, have been demonstrated to be the dominant mechanism of dissipation [16]- [19]. Considering the vortex entry potential obtained in [18], we can write the zero bias resistance of the wire as:…”
Section: Ozone Treatment On Ybco Nanowiresmentioning
confidence: 99%