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Download e-book for iPad: High-temperature Superconductivity in Cuprates: The by A. Mourachkine

By A. Mourachkine

ISBN-10: 1402008104

ISBN-13: 9781402008108

“The Frontiers of Knowhledge (to coin a word) are continually at the movement. - day’s discovery will day after today be a part of the psychological furnishings of each learn employee. through the tip of subsequent week it will likely be in each process graduate lectures. in the month there'll be a clamour to have it within the undergraduate c- riculum. subsequent 12 months, I do think, it's going to appear so regular that it can be assumed to be identified by means of each schoolboy. “The means of advancing the road of settlements, and cultivating and c- ilizing the hot territory, occurs in phases. the unique papers are p- lished, to the pride in their authors, and to the serious eyes in their readers. overview articles then offer crude cartoon plans, straight forward courses in the course of the forests of the literature. Then come the monographs, targeted surveys, mapping out the floor that has been received, adjusting claims for precedence, placing each one truth or thought into its position” (J. M. Ziman, ideas of the idea of Solids (Cambridge college Press, 1972) p.v). the most function of the publication is to provide the mechanism of - perconductivity chanced on in 1986 via J. G. Bednorz and okay. A. Müller, and to debate the physics of superconductors. The final bankruptcy of the ebook offers research of tunneling measurements in cuprates. The booklet is - dressed to researchers and graduate scholars in all branches of actual sciences.

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Additional resources for High-temperature Superconductivity in Cuprates: The Nonlinear Mechanism and Tunneling Measurements

Example text

The lattice constants are and This compound is often termed the 214 structure, because it has two La (Sr), one Cu and four O atoms. Upon examining the unit cell, Fig. 2a reveals that the basic 214 structure is doubled to form a unit cell. Therefore a more proper label might be 428. The reason for this doubling is that every other plane is offset by one-half a lattice constant, so that the unit cell would not be truly repetitive if we stopped counting after one cycle of the atoms. 6 Å apart, separated by two LaO planes which form the charge reservoir that captures electrons from the conducting planes upon doping.

5, one can see that, at there is a plateau at This is the so-called 60 K plateau. There are two different explanations for the origin of the 60 K plateau: the hole concentration in planes at remains unchanged, and the change of hole concentration occurs exclusively in Cu–O chain layers. The second explanations is that this plateau relates directly to the anomaly in LSCO. 6 shows the unit cell of Bi-2212 which has the maximum of 95 K. The dimensions of the tetragonal lattice constants of Bi2212 are and In addition to the double layer intercalated by Ca, the unit cell also contains two semiconducting BiO and two insulating SrO layers, as shown in Fig.

McMillan [2] extended this result to the case of strong-coupling superconductors, and obtained Here the Debye temperature is used as the typical phonon frequency. 4). In BCS-McMillan’s expression for the Debye temperature occurs not only in the pre-exponential factor in the expression but also in the electron-phonon coupling constant which can be presented as where C is a constant for a given class of materials, M is the mass, and is the mean-square average phonon frequency, and Consequently, in BCS-type superconductors, increases as decreases.

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High-temperature Superconductivity in Cuprates: The Nonlinear Mechanism and Tunneling Measurements by A. Mourachkine


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