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

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...

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Veröffentlicht in:Scientific reports 2019-06, Vol.9 (1), p.1-13, Article 9274
Hauptverfasser: Solovjov, A. L., Petrenko, E. V., Omelchenko, L. V., Vovk, R. V., Goulatis, I. L., Chroneos, A.
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Chroneos, A.
description 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 ≈ 0.3 near T c that is a common value for high-temperature superconductors.
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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. 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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. 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L.</au><au>Petrenko, E. V.</au><au>Omelchenko, L. V.</au><au>Vovk, R. V.</au><au>Goulatis, I. L.</au><au>Chroneos, A.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Effect of annealing on a pseudogap state in untwinned YBa2Cu3O7−δ single crystals</atitle><jtitle>Scientific reports</jtitle><stitle>Sci Rep</stitle><date>2019-06-25</date><risdate>2019</risdate><volume>9</volume><issue>1</issue><spage>1</spage><epage>13</epage><pages>1-13</pages><artnum>9274</artnum><issn>2045-2322</issn><eissn>2045-2322</eissn><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 &lt;n ↑ n ↓ &gt; ≈ 0.3 near T c that is a common value for high-temperature superconductors.</abstract><cop>London</cop><pub>Nature Publishing Group UK</pub><pmid>31239510</pmid><doi>10.1038/s41598-019-45286-w</doi><tpages>13</tpages><oa>free_for_read</oa></addata></record>
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subjects 639/301/1005/1007
639/301/119/1003
Annealing
Crystals
Humanities and Social Sciences
multidisciplinary
Oxygen
Science
Science (multidisciplinary)
Single crystals
Stoichiometry
Temperature
Temperature effects
title Effect of annealing on a pseudogap state in untwinned YBa2Cu3O7−δ single crystals
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