Explanation of the dissipation observed in several high-temperature superconductors using a modified Ambegaokar-Halperin model
R. J. Soulen, Jr., T. L. Francavilla, W. W. Fuller-Mora, M. M. Miller, C. H. Joshi, W. L. Carter, A. J. Rodenbush, M. D. Manlief, D. Aized
DOI 10.1103/PhysRevB.50.478 · Physical Review B
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Abstract
We have measured the current-voltage (I-V) characteristics of several high-temperature-superconducting materials with widely different morphologies (bulk Ag/Pb-Bi-Sr-Ca-Cu-O tapes, thin films of Y-Ba-Cu-O, and melt-textured, bulk Y-Ba-Cu-O samples). The I-V curves were taken at several magnetic fields ranging from 0 to 8 T. The measurements were carried out at three temperatures (4.2, 27, and 77 K) where the samples were immersed in liquid cryogens to ensure good thermal equilibrium. We compared our experimental results to the predictions of dissipation in superconductors made by the following physical models: modified Ambegaokar-Halperin, flux creep, vortex glass, collective flux creep, and a power law. The fits were extremely good for the first model and were not nearly as good for the others. Using the modified Ambegaokar-Halperin model, the critical current Ic, the normal-state resistance Rn, and γ, which is proportional to the pinning potential U(H,T), were obtained for each material. Since the Ambegaokar-Halperin model is the only one which uniquely defines Ic, we conclude that its use puts this parameter on a solid physical basis.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| YBa2Cu3O7 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| Bi2.2Sr2Ca0.8Cu2O8 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| Bi1.7Pb0.2Sb0.1Sr2Ca2Cu3O10 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| Bi2Sr2Ca2Cu3O10 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| Bi1.8Pb0.3Sr1.9Ca2Cu3.1O10 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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