1985
DOI: 10.1109/tmag.1985.1063727
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An in depth characterization of (NbTa)<inf>3</inf>Sn filamentary superconductor

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Cited by 60 publications
(45 citation statements)
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“…In this context, the difference between n and m in the prefactors for the scaling law (equations (3) and (4)) is attributed to the temperature and strain dependence of kappa. In the Kramer analysis which assumes that p = 0.5 and q = 2, the exponent of B C2 is close to 5/2 as observed in variable-temperature data on (NbTa) 3 Sn at zero strain [35]. An important feature of the functional form is that the primary multiplicative constant (i.e.…”
Section: Discussionmentioning
confidence: 62%
See 1 more Smart Citation
“…In this context, the difference between n and m in the prefactors for the scaling law (equations (3) and (4)) is attributed to the temperature and strain dependence of kappa. In the Kramer analysis which assumes that p = 0.5 and q = 2, the exponent of B C2 is close to 5/2 as observed in variable-temperature data on (NbTa) 3 Sn at zero strain [35]. An important feature of the functional form is that the primary multiplicative constant (i.e.…”
Section: Discussionmentioning
confidence: 62%
“…Average values of p and q as a function of temperature for the Nb 3 Al strand from the fits to the data in the strain range −1.79% ε 0.67% where B C2 is constrained by resistivity measurement. (T , ε), an empirical relation for κ has been found of the form [35,69]…”
Section: A Single Scaling Lawmentioning
confidence: 99%
“…The materials with the lowest c / DSc are polycrystalline materials, including MgB2 [81] and A15 materials [66,67,82,83]. Although removing high angle grain boundaries from technological polycrystalline materials is the favoured route to increase c , so far, this approach has proven very expensive.…”
Section: Resultsmentioning
confidence: 99%
“…13 The main contribution of Kramer's original theoretical work was to explain how the universal scaling of F P , which had been well established experimentally at that time, could arise. However, the details of the theory are not reliable since Kramer used an incorrect FLL shear modulus ͑C 66 ͒, which when corrected gives the wrong field dependence 14 for J C . For simplicity, he also considered a two-dimensional ͑2D͒ system and assumed that the fluxons that sheared past stationary ͑pinned͒ fluxons were in a perfectly ordered hexagonal FLL.…”
mentioning
confidence: 99%