Publicación: Effect of Ni doping on vortex pinning in CaK(Fe1-xNix)4As4 single crystals
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Fil.: Haberkorn, N. Comisión Nacional de Energía Atómica. Instituto Balseiro; Argentina; Universidad Nacional de Cuyo; Argentina; Consejo Nacional de Investigaciones Científicas y Técnicas; Argentina; Iowa State University. U.S. Department of Energy. Ames Laboratory; Estados Unidos
Fil.: Xu, M. Iowa State University. U.S. Department of Energy. Ames Laboratory; Estados Unidos; Iowa State University. Department of Physics and Astronomy; Estados Unidos
Fil.: Meier, W. R. Iowa State University. U.S. Department of Energy. Ames Laboratory; Estados Unidos; Iowa State University. Department of Physics and Astronomy; Estados Unidos
Fil.: Schmidt, J. Universidad de Buenos Aires. Instituto de Física de Buenos Aires. Consejo Nacional de Investigaciones Científicas y Técnicas. Facultad de Ciencias Exactas y Naturales. Departamento de Física; Argentina; Iowa State University. U.S. Department of Energy. Ames Laboratory; Estados Unidos
Fil.: Bud’ko, S. L. Iowa State University. U.S. Department of Energy. Ames Laboratory; Estados Unidos; Iowa State University. Department of Physics and Astronomy; Estados Unidos
Fil.: Canfield, P. C. Iowa State University. U.S. Department of Energy. Ames Laboratory; Estados Unidos; Iowa State University. Department of Physics and Astronomy; Estados Unidos
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Centro Atómico Bariloche
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eng
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We study the correlation between chemical composition and vortex dynamics in Ni-doped CaK(Fe1−xNix)4As4 (x=0, 0.015, 0.025, 0.03, and 0.05) single crystals by performing measurements of the critical current densities Jc and the flux creep rates S. The magnetic relaxation of all the crystals is well described by the collective creep theory. The samples display a glassy exponent μ within the predictions for vortex bundles in a weak pinning scenario and relatively small characteristic pinning energy (U0<100K). The undoped crystals display modest Jc values at low temperatures and high magnetic fields applied along the c axis. Jc(T) dependences at high fields display an unusual peak. The enhancement in Jc(T) matches with an increase in U0 and the appearance of a second peak in the magnetization. As Ni doping increases, whereas there is a monotonic decrease in Tc there is a nonmonotonic change in Jc. Initially Jc increases, reaching a maximum value for x=0.015, and then Jc decreases for x≥0.025. This change in Jc(x) is coincident with the onset of antiferromagnetic order. The magnetic field dependence of Jc(H) also manifests a change in behavior between these x values. The analysis of the vortex dynamics for small and intermediate magnetic fields shows a gradual evolution in the glassy exponent μ with Ni content, x. This implies that there is no appreciable change in the mechanism that determines the vortex relaxation.
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Physical Review B. Vol. 100, no. (2019), p. 064524