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首页> 外文期刊>Journal of Superconductivity and Novel Magnetism >On the Role of Fermi Energy in Determining Properties of Superconductors: a Detailed Comparative Study of Two Elemental Superconductors (Sn and Pb), a Non-cuprate (MgB 2 ) and Three Cuprates (YBCO, Bi-2212 and Tl-2212)
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On the Role of Fermi Energy in Determining Properties of Superconductors: a Detailed Comparative Study of Two Elemental Superconductors (Sn and Pb), a Non-cuprate (MgB 2 ) and Three Cuprates (YBCO, Bi-2212 and Tl-2212)

机译:关于费米能量在确定超导体性能中的作用:两种元素超导体(Sn和Pb),一种非铜酸盐(MgB 2)和三种铜酸盐(YBCO,Bi-2212和Tl-2212)的详细比较研究

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摘要

Fermi energies (E (F)s) of high- T (c) superconductors (SCs) have of late been evincing considerable interest because they are believed to be the cause of their high T (c)s and gap structures. Since Bardeen-Cooper-Schrieffer (BCS) equations for elemental and generalized-BCS equations for non-elemental SCs are derived under the blanket of the assumption E (F)/ k theta > > 1 (k = Boltzmann constant, theta = Debye temperature), they cannot shed light on the E (F)s of these SCs. This fact leads us to address the gaps (Delta(0)s) and T (c)s of both types of SCs via recently derived equations which incorporate E (F) as a variable. For the specification of the E (F) of any SC, we now need another of its properties. Choosing j (0), the critical current density of the SC at T = 0, and following an idea due to Pines, we present for both types of SCs new equations for j (0) that depend solely on the following properties of the SC: E (F), theta, gram-atomic volume, electronic specific heat constant and a dimensionless construct where m* is the effective mass of superconducting electrons and P (0) their critical momentum. Appeal to the experimental values of Delta(0), T (c) and j (0) of any SC then not only leads to values of E (F), m* and P (0) but also provides plausible clues about how its j (0)-and therefore T (c)-may be increased.
机译:高T(c)超导体(SC)的费米能(E(F))最近引起了人们的极大兴趣,因为它们被认为是其高T(c)和间隙结构的原因。由于用于非元素SC的元素的Bardeen-Cooper-Schrieffer(BCS)方程和用于非元素SC的广义BCS方程是在假设E(F)/ k theta 1(k =玻尔兹曼常数,theta =德拜温度)的前提下得出的),则无法了解这些SC的E(F)。这一事实使我们能够通过将E(F)作为变量的最近导出的方程式来解决两种类型的SC的间隙(Delta(0)s和T(c)s。对于任何SC的E(F)的规范,我们现在都需要它的另一个属性。选择j(0),即T = 0时SC的临界电流密度,并根据Pines的想法,针对两种类型的SC提出j(0)的新方程,其仅取决于SC的以下特性:E(F),θ,克原子体积,电子比热常数和无量纲构造,其中m *是超导电子的有效质量,P(0)是其临界动量。吸引任何SC的Delta(0),T(c)和j(0)的实验值,不仅可以得出E(F),m *和P(0)的值,而且可以提供有关其j(0)-因此T(c)-可能会增加。

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