1981
DOI: 10.6089/jscm.7.74
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Cited by 15 publications
(18 citation statements)
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“…In fact, they are not far from the BCS to BE crossover, defined as shown by Pistolesi and Strinati by the condition (k F ξ pair ) = 1. One of the manifestations of this proximity is the Uemura plot T c ∝ λ −2 followed by all underdoped cuprates (Uemura, 2002). Another one is the observation of strong fluctuation effects in the heat capacity transition.…”
Section: Some Comments On the Pseudogapmentioning
confidence: 99%
“…In fact, they are not far from the BCS to BE crossover, defined as shown by Pistolesi and Strinati by the condition (k F ξ pair ) = 1. One of the manifestations of this proximity is the Uemura plot T c ∝ λ −2 followed by all underdoped cuprates (Uemura, 2002). Another one is the observation of strong fluctuation effects in the heat capacity transition.…”
Section: Some Comments On the Pseudogapmentioning
confidence: 99%
“…Another interesting point concerning this material is that some experiments suggest possible occurrence of an unconventional superconductivity, [2 -5] although there are also experiments suggesting conventional pairing [6]. In particular, an unchanged Knight shift across T c found in some experiments suggests spin-triplet pairing [3], while absence of broken time reversal symmetry [7,8] may exclude possibility of chiral p-wave or d-wave pairing states, leaving spin-triplet f-wave pairing as a good candidate.…”
mentioning
confidence: 99%
“…Since the nodes of the f-wave gap intersects the large Fermi surface, this can account for the experimental results suggesting the existence of gap nodes. In fact, it has recently been found that a muon spin relaxation data can be well explained by taking this view [8]. Another point to be mentioned in relation with the experiments is that the pocket Fermi surfaces are not observed in angle-resolved photoemission spectroscopy (ARPES) experiments [29,30] up to date.…”
mentioning
confidence: 99%
“…The magnetic field penetration depth λ of superconductors is related to the superconducting carrier density n s divided by the effective mass m * as 1/λ 2 ∝ n s /m * . In a recent paper Uemura [27] explained the experimental data found in [28] assuming a microscopic phase separation between superfluid and non-superconducting fermionic carriers, similar to the superfluid He films. Recently, it was reported that, the photoemission spectra near the Brillouin zone boundary, exhibit unexpected sensitivity to the superfluid density [29], supporting the universality as function of doping and temperature of the properties of the cuprates.…”
Section: Resultsmentioning
confidence: 99%
“…We calculated the London penetration depth and the c-axis and ab-plane conductivity and compared the results with the experimental data. The study of experimental dependence of the penetration depth is an important problem [27,28].…”
Section: Discussionmentioning
confidence: 99%