Pinning phenomena and critical currents in disordered long Josephson junctions
Roland Fehrenbacher, Vadim B. Geshkenbein, Gianni Blatter
DOI 10.1103/PhysRevB.45.5450 · Physical Review B
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Abstract
The critical current Ic of a long one-dimensional (1D) Josephson junction in the presence of different types of structural disorder is investigated both analytically and numerically. It is shown that most properties of Ic can be understood from the behavior of the elementary pinning force (PF) of a single defect, which we calculate exactly as a function of the external magnetic field He, pinning-center size, and strength. The following types of disorder are discussed: (i) For a given field, and pinning centers with equal strength, a unique arrangement of pins that maximizes Ic is found. (ii) In the case of a periodic pinning-center lattice, we reproduce the commensurability peaks in the field dependence of the critical current, Ic(He), previously reported by Oboznov and Ustinov [Phys. Lett. A 139, 481 (1989)]. In addition, we predict that a peak can be damped or disappear, if its position coincides with a field value at which the elementary PF vanishes. (iii) The most interesting effects appear in the presence of random disorder. Using the exact expression for the elementary PF, we extend the collective pinning analysis of Koshelev and Vinokur (Zh. Eksp. Teor. Fiz. 97, 976 (1990) [Sov. Phys. JETP 70, 547 (1990)]) to arbitrary fields and properties of the disorder, and compare the obtained predictions with the results of numerical simulations. The agreement between the two approaches is extremely good. In particular, we find that the appearance of a plateau in Ic(He) for large fields depends strongly on the ratio r¯0/λ¯j between the average pinning center size r¯0 and the average Josephson penetration depth λ¯j. If r¯0/λ¯j≊1, there is no plateau at all, and in the case r¯0/λ¯j≪1, a plateau is found up to fields for which the vortex spacing becomes of the order of r¯0. Furthermore, we predict the possibility of a dimensional crossover from a 1D behavior at low fields to 0D behavior at large fields. Finally, we present a possible explanation of the experimentally observed plateau in the jc(He) dependence of granular high-Tc materials.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| YBa2Cu3O7-δ Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
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