1998
DOI: 10.1103/physrevb.58.132
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Anisotropy dependence of half-loop-mediated vortex motion in thallium-based superconductors studied by magnetoresistivity

Abstract: By measuring the temperature dependence of the magnetoresistivity, we have studied the activation energy U of two Tl-based superconducting oxides having different electronic anisotropies ͑Tl-2212, which is very anisotropic, close to Bi-2212, and Tl-1212, the anisotropy of which is about 10͒. The activation energies are described in terms of movements of half loops of vortices, with a lateral size of about the intervortex spacing a 0 . Taking into account the field dependence of the elastic coefficients C 44 an… Show more

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Cited by 16 publications
(9 citation statements)
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“…More interestingly, Q exhibits a clear square-root ac field dependence, which is emphasized in figure 4(top) by plotting Q H −1/2 ac vs. T . This dependence is expected for dislocation-mediated plastic flux creep where vortices propagate by protruding vortex half-loops into local energy minima in the vortex ensemble, and has previously been observed at higher fields in other anisotropic materials such as Bi 2 Sr 2 CaCu 2 O 8+x (Bi-2212) thin films, Tl 2 Ba 2 CaCu 2 O 8 (Tl-2212) single crystals [29,30] and Tl 2/3 Ba 1/3 Sr 2 CaCu 2 O 7 (Tl-1212) single crystals [30]. The barrier limiting this vortex motion is roughly given by the creation energy of a vortex-antivortex pair perpendicular to the original vortex [31] …”
Section: Resultssupporting
confidence: 60%
“…More interestingly, Q exhibits a clear square-root ac field dependence, which is emphasized in figure 4(top) by plotting Q H −1/2 ac vs. T . This dependence is expected for dislocation-mediated plastic flux creep where vortices propagate by protruding vortex half-loops into local energy minima in the vortex ensemble, and has previously been observed at higher fields in other anisotropic materials such as Bi 2 Sr 2 CaCu 2 O 8+x (Bi-2212) thin films, Tl 2 Ba 2 CaCu 2 O 8 (Tl-2212) single crystals [29,30] and Tl 2/3 Ba 1/3 Sr 2 CaCu 2 O 7 (Tl-1212) single crystals [30]. The barrier limiting this vortex motion is roughly given by the creation energy of a vortex-antivortex pair perpendicular to the original vortex [31] …”
Section: Resultssupporting
confidence: 60%
“…( 1). The value of 380 is comparable to the typical values which were recently found for the overdoped (γ = 360-490), the optimally doped (γ = 550) and the slightly underdoped (γ = 800) BSCCO single crystals as well [9,17,18]. The same analysis for BPSCCO single crystals brings out a value of γ of 60 (fig.…”
supporting
confidence: 82%
“…In this letter, we present a comparative study between BSCCO, Bi 1.8 Pb 0.2 Sr 2 CaCu 2 O 8+δ (BPSCCO) and (K, Ba)BiO 3 (KBBO) compounds using the same technique as proposed before by Warmont et al [9] to determine the anisotropy factor. The Pb doping in BSCCO indeed increases the carrier concentration and causes a shift to the overdoped region in the phase diagram [10].…”
mentioning
confidence: 99%
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“…In the linear temperature range, the extracted activation energy is then U act (T,B)ϭU 0 (B)͓1ϪT/T c ͔. For a 3D vortex loops model, 31,33 the expression of the activation energy is U loop (T,B) ϭ ͓␣ 0…”
Section: Resultsmentioning
confidence: 99%