A. L. Solovjov, K. Rogacki, N. V. Shytov, E. V. Petrenko, L. V. Bludova, A. Chroneos, R. V. Vovk
{"title":"Influence of strong electron irradiation on fluctuation conductivity and pseudogap in YBa2Cu3O7−δ single crystals","authors":"A. L. Solovjov, K. Rogacki, N. V. Shytov, E. V. Petrenko, L. V. Bludova, A. Chroneos, R. V. Vovk","doi":"10.1103/physrevb.111.174508","DOIUrl":null,"url":null,"abstract":"The effect of high-energy electron irradiation on the temperature dependences of the resistivity ρ(), fluctuation conductivity (FLC), and pseudogap (PG) Δ*() of YB</a:mi>a</a:mi>2</a:mn></a:msub>C</a:mi>u</a:mi>3</a:mn></a:msub>O</a:mi>7</a:mn>−</a:mo>δ</a:mi></a:mrow></a:msub></a:mrow></a:math> (YBCO) single crystals containing virtually no twins was studied. A linear increase in the resistivity and a linear decrease in the superconducting (SC) transition temperature <f:math xmlns:f=\"http://www.w3.org/1998/Math/MathML\"><f:msub><f:mi>T</f:mi><f:mi>c</f:mi></f:msub></f:math> with increasing irradiation doses φ were observed. For relatively small φ, the linear <g:math xmlns:g=\"http://www.w3.org/1998/Math/MathML\"><g:msub><g:mi>T</g:mi><g:mi>c</g:mi></g:msub></g:math> can be described by the Abrikosov-Gorkov (AG) pair breaking theory, and for large φ, by the Emery-Kivelson (EK) theory, which takes into account the suppression of <h:math xmlns:h=\"http://www.w3.org/1998/Math/MathML\"><h:msub><h:mi>T</h:mi><h:mi>c</h:mi></h:msub></h:math> by quantum phase fluctuations caused by irradiation defects. As FLC shows, at the average value of <i:math xmlns:i=\"http://www.w3.org/1998/Math/MathML\"><i:mrow><i:msub><i:mi>φ</i:mi><i:mn>3</i:mn></i:msub><i:mo>=</i:mo><i:mn>2.5</i:mn><i:mo>×</i:mo><i:msup><i:mrow><i:mn>10</i:mn></i:mrow><i:mn>19</i:mn></i:msup><i:mspace width=\"0.16em\"/><i:mi mathvariant=\"normal\">e</i:mi><i:mo>/</i:mo><i:mi mathvariant=\"normal\">c</i:mi><i:msup><i:mrow><i:mi mathvariant=\"normal\">m</i:mi></i:mrow><i:mn>2</i:mn></i:msup></i:mrow></i:math>, which corresponds to the AG-EK crossover, the distance between the conducting <n:math xmlns:n=\"http://www.w3.org/1998/Math/MathML\"><n:mrow><n:mi>Cu</n:mi><n:msub><n:mi mathvariant=\"normal\">O</n:mi><n:mn>2</n:mn></n:msub></n:mrow></n:math> planes, <p:math xmlns:p=\"http://www.w3.org/1998/Math/MathML\"><p:msub><p:mi>d</p:mi><p:mn>01</p:mn></p:msub></p:math>, as well as the coherence lengths along the <q:math xmlns:q=\"http://www.w3.org/1998/Math/MathML\"><q:mi>c</q:mi></q:math> axis, <r:math xmlns:r=\"http://www.w3.org/1998/Math/MathML\"><r:msub><r:mi>ξ</r:mi><r:mi mathvariant=\"normal\">c</r:mi></r:msub></r:math>(0), and the region of SC fluctuations, <t:math xmlns:t=\"http://www.w3.org/1998/Math/MathML\"><t:mrow><t:mi mathvariant=\"normal\">Δ</t:mi><t:msub><t:mi>T</t:mi><t:mi>fl</t:mi></t:msub></t:mrow></t:math>, increase sharply, and the two-dimensional contribution of the Maki-Thompson fluctuations (2D-MT) unexpectedly changes to the two-dimensional contribution of the Aslamazov-Larkin (2D-AL). Surprisingly, no features in ρ(φ) and <v:math xmlns:v=\"http://www.w3.org/1998/Math/MathML\"><v:msub><v:mi>T</v:mi><v:mi>c</v:mi></v:msub></v:math>(φ) indicating the AG-EK crossover are observed. At the same time, at <w:math xmlns:w=\"http://www.w3.org/1998/Math/MathML\"><w:msub><w:mi>φ</w:mi><w:mn>3</w:mn></w:msub></w:math>, a sharp increase in the opening temperature of PG, *, as well as the value of PG, Δ*, is observed, which indicates a possible decrease in DOS under the influence of defects. With a further increase in φ, all the parameters of PG and its dimensions are greatly reduced, and an unusual shape of Δ*() is found. However, quite unexpectedly, at <x:math xmlns:x=\"http://www.w3.org/1998/Math/MathML\"><x:mrow><x:msub><x:mi>φ</x:mi><x:mn>5</x:mn></x:msub><x:mo>=</x:mo><x:mn>5.6</x:mn><x:mo>×</x:mo><x:msup><x:mrow><x:mn>10</x:mn></x:mrow><x:mn>19</x:mn></x:msup><x:mspace width=\"0.16em\"/><x:mi mathvariant=\"normal\">e</x:mi><x:mo>/</x:mo><x:mi mathvariant=\"normal\">c</x:mi><x:msup><x:mrow><x:mi mathvariant=\"normal\">m</x:mi></x:mrow><x:mn>2</x:mn></x:msup></x:mrow></x:math> the temperature dependences of both FLC and PG demonstrate curves typical for well-structured YBCO, regardless of the number of defects. <jats:supplementary-material> <jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement> <jats:copyright-year>2025</jats:copyright-year> </jats:permissions> </jats:supplementary-material>","PeriodicalId":20082,"journal":{"name":"Physical Review B","volume":"43 1","pages":""},"PeriodicalIF":3.7000,"publicationDate":"2025-05-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physical Review B","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1103/physrevb.111.174508","RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"Physics and Astronomy","Score":null,"Total":0}
引用次数: 0
Abstract
The effect of high-energy electron irradiation on the temperature dependences of the resistivity ρ(), fluctuation conductivity (FLC), and pseudogap (PG) Δ*() of YBa2Cu3O7−δ (YBCO) single crystals containing virtually no twins was studied. A linear increase in the resistivity and a linear decrease in the superconducting (SC) transition temperature Tc with increasing irradiation doses φ were observed. For relatively small φ, the linear Tc can be described by the Abrikosov-Gorkov (AG) pair breaking theory, and for large φ, by the Emery-Kivelson (EK) theory, which takes into account the suppression of Tc by quantum phase fluctuations caused by irradiation defects. As FLC shows, at the average value of φ3=2.5×1019e/cm2, which corresponds to the AG-EK crossover, the distance between the conducting CuO2 planes, d01, as well as the coherence lengths along the c axis, ξc(0), and the region of SC fluctuations, ΔTfl, increase sharply, and the two-dimensional contribution of the Maki-Thompson fluctuations (2D-MT) unexpectedly changes to the two-dimensional contribution of the Aslamazov-Larkin (2D-AL). Surprisingly, no features in ρ(φ) and Tc(φ) indicating the AG-EK crossover are observed. At the same time, at φ3, a sharp increase in the opening temperature of PG, *, as well as the value of PG, Δ*, is observed, which indicates a possible decrease in DOS under the influence of defects. With a further increase in φ, all the parameters of PG and its dimensions are greatly reduced, and an unusual shape of Δ*() is found. However, quite unexpectedly, at φ5=5.6×1019e/cm2 the temperature dependences of both FLC and PG demonstrate curves typical for well-structured YBCO, regardless of the number of defects. Published by the American Physical Society2025
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