Titlebook: New Trends in Superconductivity; James F. Annett,Sergei Kruchinin Book 2002 Springer Science+Business Media Dordrecht 2002 Doping.HTS.Jose

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Palter

Growth of a Hard-Grown Single Crystal — Bi2Sr2Ca2Cu3O10+ðl growth conditions, such as, an extremely slow growing rate at ∼0.04 mm/h, a sharp temperature gradient of ∼300 °C/cm, growth atmosphere using mixed gases of 20% oxygen and 80% argon and post-growth annealing in flowing oxygen, were investigated in order to obtain large and high quality of the crys

RENIN

Exchange and Spin-Fluctuation Pairing in the Two-Band Hubbard Model be responsible for the high values of T. [.], A distinctive feature of high-T. copper oxide superconductors is strong antiferromagnetic (AFM) exchange interaction (see, for example, [.]). The exchange binding energy of two holes with spin 1/2 in copper Cu(3.) and oxygen O(2.)ions comprises a value

大喘气

High Temperature Superconductors in High Frequency Fields expected by anybody familiar with the history of superconductvity, the path to marketable products has proved to be extremely arduous. However, due to an unprecedented effort in research and development some technologically viable products have already reached the market. Notable among these are hi

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Stripe-Like Inhomogeneities, Carriers, and BCS-BEC Crossover in the High-,, Cupratesl stripe-like inhomogeneities, where narrow charged stripes form antiphase domain walls separating wider antiferromagnetic (AF) stripes. Experimental observations have been pointing to the presence of both itinerant and almost localized (or polaron-like) carriers in the cuprates. First-principles ca

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Charge- and Spin-Density-Wave Superconductors: Pseudogap Puzzle in the Cuprates and SDWs (hereafter we shall also use the abbreviation DWs for a common case) correspond to the so-called diagonal long-range order (DLRO), as distinct from superconductors. For the latter a two-particle density matrix, characterizing the superconducting state, can be factorized into a product of t

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Strong-Coupling Superconductivity with D-Wave Order Parameter and S-Wave Gapctron repulsive correlations. However, assessing the role of different interactions in novel superconductors one has to take into account that these materials are highly polarizable ionic lattices, where the Fröhlich electron-phonon interaction with optical phonons should be strong. Indeed, a parame

averse

Theory of BSCCO Bicrystal ,-Axis Twist Josephson Junctions: A New Phase-Sensitive Test of Order Parates. Although there are many experiments that suggest the possibility of line nodes of the OP, most of these experiments are not sensitive to the phase of the OP. The important question for the determining whether a new type of pairing mechanism is really necessary is to decide if the OP really is o

淘气

Time Reversal Breaking States and Spontaneous Current Pattern in Josephson Junctions of D-Wave Super last years both in theory and experiment (see reviews [., .]). Several mechanisms of Τ-breaking and corresponding spontaneous currents generation have been proposed and studied, particularly: appearance of a subdominant order parameter and the proximity effect. The latter case is realized, in parti

hauteur

Electronic Thermal Conductivity of Partially-Gapped CDW Superconductorsuperconducting critical temperature T. [., ., .]. On the contrary, the lattice thermal conductivity κ. grows with decreasing temperature, T; the larger phonon mean free path stemming from the exponential drop of the quasiparticle number for T → 0. Therefore, the overall quantity κ(T) = κ.(T) + κ.(T)