1997
DOI: 10.1103/physrevlett.79.135
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Nonlocal Effects on the Magnetic Penetration Depth ind-Wave Superconductors

Abstract: We show that, under certain conditions, the low temperature behavior of the magnetic penetration depth λ(T ) of a pure d-wave superconductor is determined by nonlocal electrodynamics and, contrary to the general belief, the deviation ∆λ(T ) = λ(T ) − λ(0) is proportional to T 2 and not T . We predict that the ∆λ(T ) ∝ T 2 dependence, due to nonlocality, should be observable experimentally in nominally clean high-Tc superconductors below a crossover temperature T * = (ξo/λo) ∆o ∼ 1K. Possible complications due … Show more

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Cited by 174 publications
(202 citation statements)
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“…Kosztin and Leggett [119] first pointed out that since the BCS coherence length defined as , the two processes would be difficult to distinguish. However, unlike the effect from impurities, the predicted nonlocality is dependent upon the orientation of the magnetic field and sample boundaries.…”
Section: Nonlocal Electrodynamics Of Nodal Superconductorsmentioning
confidence: 99%
“…Kosztin and Leggett [119] first pointed out that since the BCS coherence length defined as , the two processes would be difficult to distinguish. However, unlike the effect from impurities, the predicted nonlocality is dependent upon the orientation of the magnetic field and sample boundaries.…”
Section: Nonlocal Electrodynamics Of Nodal Superconductorsmentioning
confidence: 99%
“…5 . This presents a conundrum-mechanisms such as impurity pair-breaking 20,21 and nonlocal electrodynamics 22 should cause a crossover to quadratic temperature dependence, but attempts to understand the behaviour in terms of impurity physics require unrealistically high levels of disorder 23 . Measurements of the frequency-dependent superfluid density offer the potential for new insights into this problem.…”
mentioning
confidence: 99%
“…1 More recently the concept of nonlocality was applied to high-T c cuprates. 2 In the nonlocal theory B͑z͒ deviates from a simple exponential decay; it is nonmonotonic and, moreover, changes sign at a specific depth. 1 In the pure limit ͑ 0 Ӷ ᐉ͒ B͑z͒ is a function of the intrinsic parameters L ͑T =0͒ and 0 , and the temperature T. The magnitude of this nonlocal effect is determined by the ratio 0 / L ͑0͒ ϰ 1 / ; the smaller the Ginzburg-Landau parameter , the bigger the nonlocal effect.…”
mentioning
confidence: 99%