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Effect of annealing on a pseudogap state in untwinned YBa2Cu3O7−δ single crystals

A. L. SolovjovB. I. Verkin Institute for Low Temperature Physics and Engineering of National Academy of Science of Ukraine, 47 Nauki ave., 61103, Kharkov, UkraineE. V. PetrenkoB. I. Verkin Institute for Low Temperature Physics and Engineering of National Academy of Science of Ukraine, 47 Nauki ave., 61103, Kharkov, UkraineL. V. OmelchenkoB. I. Verkin Institute for Low Temperature Physics and Engineering of National Academy of Science of Ukraine, 47 Nauki ave., 61103, Kharkov, UkraineР. В. ВовкPhysics Department, V. Karazin Kharkiv National University, Svobody Sq. 4, 61077, Kharkiv, UkraineΙ. L. GoulatisPhysics Department, V. Karazin Kharkiv National University, Svobody Sq. 4, 61077, Kharkiv, UkraineA. ChroneosDepartment of Materials, Imperial College, London, SW7 2AZ, UK. [email protected]
2019en
ABI

Аннотация

Abstract The effect of annealing both in the oxygen atmosphere and at room temperatures on physical properties such as the pseudogap (Δ*(T)) and excess conductivity (σ′(T)) of untwined YBa 2 Cu 3 O 7−δ (YBCO) single crystal with a small deviation from oxygen stoichiometry is studied. It was revealed that as the charge carrier density, n f , increases, Т с also slightly increases, whereas the temperature of the pseudogap opening, T*, decreases noticeably, which is consistent with the phase diagram (PD) of cuprates. The excess conductivity in the vicinity of T c is represented by the Aslamazov-Larkin and Hikami-Larkin fluctuation theories, illustrating the three-dimensional to two-dimensional (i.e. 3D-2D) crossover with an increase in temperature. The crossover temperature T 0 determines the coherence length along the c axis is ξ c (0) = 0.86 Å, that is 2.6 times larger than for optimally doped YBCO single crystals with defects. Taking into account the short coherence length in high-temperature superconductors, in the model of free charge carriers the phase relaxation time of fluctuating Cooper pairs is determined, τ φ (100 K) = (4.55 ± 0.4) · 10 −13 s, which is slightly (1.2 times) larger than in well-structured YBCO films, and as in films, does not depend on n f . It is shown that Δ*(T) at different annealing stages practically does not change its shape. As in the well-structured YBCO films, Δ*(T) demonstrates maximum at T pair ~124 K which depends weakly on n f . However, the maximum value of Δ*(T pair ) increases with increasing n f , as it follows from the PD of cuprates. Comparing the experimental data with the Peters-Bauer theory we estimated the density of local pairs <n ↑ n ↓ > ≈ 0.3 near T c that is a common value for high-temperature superconductors.

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