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<article dtd-version="1.3" article-type="research-article" xml:lang="en"><front xmlns:ali="http://www.niso.org/schemas/ali/1.0/" xmlns:c="http://ns.iop.org/namespaces/content" xmlns:date="http://ns.iop.org/namespaces/functions/date" xmlns:m="http://ns.iop.org/namespaces/meta" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"><journal-meta><journal-id journal-id-type="publisher-id">sust</journal-id><journal-id journal-id-type="coden">SUSTEF</journal-id><journal-title-group><journal-title>Superconductor Science and Technology</journal-title><abbrev-journal-title abbrev-type="IOP">SUST</abbrev-journal-title><abbrev-journal-title abbrev-type="publisher">Supercond. Sci. Technol.</abbrev-journal-title></journal-title-group><issn pub-type="ppub">0953-2048</issn><issn pub-type="epub">1361-6668</issn><publisher><publisher-name>IOP Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="publisher-id">sustadb6d8</article-id><article-id pub-id-type="doi">10.1088/1361-6668/adb6d8</article-id><article-id pub-id-type="manuscript">adb6d8</article-id><article-id pub-id-type="other">SUST-106634.R1</article-id><article-categories><subj-group subj-group-type="display-article-type"><subject>Paper</subject></subj-group></article-categories><title-group><article-title>Vortex dynamics study on an uniaxially textured YBCO/MgO superconducting film from magnetic measurements</article-title></title-group><contrib-group><contrib contrib-type="author" corresp="yes"><contrib-id authenticated="false" contrib-id-type="orcid">0000-0002-6211-165X</contrib-id><name name-style="western"><surname>Cornejo</surname><given-names>H Sanchez</given-names></name><xref ref-type="aff" rid="sustadb6d8af1">1</xref><xref ref-type="fn" rid="sustadb6d8fn1"><sup>*</sup></xref><email>henrysanchez45@gmail.com</email></contrib><contrib contrib-type="author"><name name-style="western"><surname>Domínguez</surname><given-names>A Bustamante</given-names></name><xref ref-type="aff" rid="sustadb6d8af1">1</xref></contrib><contrib contrib-type="author"><contrib-id authenticated="true" contrib-id-type="orcid">0000-0002-3221-5124</contrib-id><name name-style="western"><surname>Holmes</surname><given-names>S N</given-names></name><xref ref-type="aff" rid="sustadb6d8af2">2</xref></contrib><contrib contrib-type="author"><contrib-id authenticated="true" contrib-id-type="orcid">0000-0002-0366-609X</contrib-id><name name-style="western"><surname>Seo</surname><given-names>J W</given-names></name><xref ref-type="aff" rid="sustadb6d8af3">3</xref></contrib><contrib contrib-type="author"><name name-style="western"><surname>Aguiar</surname><given-names>J Albino</given-names></name><xref ref-type="aff" rid="sustadb6d8af4">4</xref></contrib><contrib contrib-type="author"><name name-style="western"><surname>Silva</surname><given-names>V A J</given-names></name><xref ref-type="aff" rid="sustadb6d8af4">4</xref></contrib><contrib contrib-type="author"><name name-style="western"><surname>Barnes</surname><given-names>C H W</given-names></name><xref ref-type="aff" rid="sustadb6d8af5">5</xref></contrib><contrib contrib-type="author" corresp="yes"><contrib-id authenticated="true" contrib-id-type="orcid">0000-0001-5930-9916</contrib-id><name name-style="western"><surname>De Los Santos Valladares</surname><given-names>L</given-names></name><xref ref-type="aff" rid="sustadb6d8af4">4</xref><xref ref-type="aff" rid="sustadb6d8af5">5</xref><xref ref-type="fn" rid="sustadb6d8fn1"><sup>*</sup></xref><email>ld301@cam.ac.uk</email></contrib><aff id="sustadb6d8af1">
<label>1</label>Laboratorio de Cerámicos y Nanomateriales, Facultad de Ciencias Físicas, <institution>Universidad Nacional Mayor de San Marcos</institution>, Ap. Postal 14-0149, Lima 14, <country>Peru</country></aff><aff id="sustadb6d8af2">
<label>2</label>Department of Electronic and Electrical Engineering, <institution>University College London</institution>, Torrington Place, London WC1E 7JE, <country>United Kingdom</country></aff><aff id="sustadb6d8af3">
<label>3</label>College of Science and Technology Convergence, <institution>Yonsei University</institution>, 1 Yonseidae-gil, Wonju, Gangwon-do, 26493, <country>Republic of Korea</country></aff><aff id="sustadb6d8af4">
<label>4</label>Programa de Pós-Graduação em Ciências de Materiais, Centro de Ciências Exatas e da Natureza, <institution>Universidade Federal de Pernambuco</institution>, 50670-901 Recife-PE, <country>Brazil</country></aff><aff id="sustadb6d8af5">
<label>5</label>Cavendish Laboratory, Department of Physics, <institution>University of Cambridge</institution>, J. J. Thomson Ave., Cambridge CB3 0HE, <country>United Kingdom</country></aff></contrib-group><author-notes><fn id="sustadb6d8fn1"><label>*</label><p>Authors to whom any correspondence should be addressed.</p></fn></author-notes><pub-date iso-8601-date="2025-03-01" pub-type="ppub"><day>01</day><month>03</month><year>2025</year></pub-date><pub-date iso-8601-date="2025-03-05" pub-type="epub"><day>05</day><month>03</month><year>2025</year></pub-date><pub-date iso-8601-date="2025-03-05" pub-type="open-access"><day>05</day><month>03</month><year>2025</year></pub-date><volume>38</volume><issue>3</issue><elocation-id content-type="artnum">035028</elocation-id><supplementary-material content-type="colour-figures" orientation="portrait" position="float"/><supplementary-material content-type="supp-data" id="SM0001" orientation="portrait" position="float" xlink:href="https://content.cld.iop.org/journals/0953-2048/38/3/035028/revision2/sustadb6d8supp1.pdf?Expires=1741778967&amp;Signature=dE3lXYhbYXacm1VEnueC35BMvoh6E-q-tpIQPDdvglA~rV2gYEb051A3S6mKnlOvaNxUuqzVnkjfTgUvsgAR1061B0ZJX~X4-ktLPDBDfYRaj5aLtYa3fKjG4xg6t9GLC0smlIfabcxFrWEmgbs3eEWZwyy00HLgZk0v~CMgwie4jlr9I8W99CZmkl97QVnRVjeTebmP68a3NWfB9V24~uDPLCcTwb~NzLUCjFEDlumKgyytB2XaKhNMg1nzVYbQFiRLTorSLn0TO293zHdZnJwpBBdA15MmE1rEoACD6gPru6eYF7otjJ2u8R06fsf-9Aq0BYY1bE3ZT-NHiWvQOQ__&amp;Key-Pair-Id=KL1D8TIY3N7T8"><label>Supplementary data</label><caption><p>(0.8 MB PDF)</p></caption></supplementary-material><history><date date-type="received"><day>27</day><month>11</month><year>2024</year></date><date date-type="rev-recd"><day>21</day><month>01</month><year>2025</year></date><date date-type="accepted"><day>17</day><month>02</month><year>2025</year></date><date date-type="oa-requested"><day>21</day><month>01</month><year>2025</year></date></history><permissions><copyright-statement>© 2025 The Author(s). Published by IOP Publishing Ltd</copyright-statement><copyright-year>2025</copyright-year><license license-type="cc-by" xlink:href="https://creativecommons.org/licenses/by/4.0/"><license-p>
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Original content from this work may be used under the terms of the <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">Creative Commons Attribution 4.0 license</ext-link>. Any further distribution of this work must maintain attribution to the author(s) and the title of the work, journal citation and DOI.</license-p></license></permissions><self-uri content-type="pdf" xlink:href="https://content.cld.iop.org/journals/0953-2048/38/3/035028/revision2/sust_38_3_035028.pdf?Expires=1741778967&amp;Signature=Ydx0O1Fjxpl7Trp67lpz4XChO~12PIht~tMgnuGI-lI~jD6AjIa1IvN0pfs8nRgLPEV~UwhTaeSVe17eocYr0vmyj6N4lbE0-jbn-7~BLxZycDza19tzv2AVqav2MK2r~TirM43499kxpmcUEcA-MGfARE6olFsjlCB2qd7f7a74kTxpaLu195K4GD6EgCG2MgyQA1y43UdIpzbmPsniGe3MXlwyKgUt4vBCGIDC3naCQDUCYRUXYBdCKfsm~-R5MudnSnphyG2lFMLm9un4sNzosRABG64i4lXiiqWtkrQYDhLVqIcDiPh14DhLso3VgFelt~0tUmMOw0MTCSHBEg__&amp;Key-Pair-Id=KL1D8TIY3N7T8"/><abstract abstract-type="standard"><title>Abstract</title><p>The vortex dynamics of an undoped uniaxially textured YBa<sub>2</sub>Cu<sub>3</sub>O<sub>7−δ</sub> (YBCO) superconducting film grown onto a MgO (100) substrate was inspected by applying the vortex glass and collective-pinning models. The texture and structural characterization studied by X-ray diffraction revealed a uniaxially (00 l) YBCO layer, which coexists with minor Y<sub>2</sub>BaCuO<sub>5</sub> and CuO phases. The temperature dependence of the magnetization in the superconducting state revealed a critical temperature <inline-formula>
<tex-math><?CDATA ${T_{\text{C}}}$?></tex-math><mml:math overflow="scroll"><mml:mrow><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mrow><mml:mtext>C</mml:mtext></mml:mrow></mml:msub></mml:mrow></mml:mrow></mml:math><inline-graphic xlink:href="https://content.cld.iop.org/journals/0953-2048/38/3/035028/revision2/sustadb6d8ieqn1.gif"/></inline-formula> = 88 K. By measuring the hysteresis loops (<inline-formula>
<tex-math><?CDATA $M\left( H \right)$?></tex-math><mml:math overflow="scroll"><mml:mrow><mml:mi>M</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>H</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:math><inline-graphic xlink:href="https://content.cld.iop.org/journals/0953-2048/38/3/035028/revision2/sustadb6d8ieqn2.gif"/></inline-formula>) at 10–70 K, the critical fields <inline-formula>
<tex-math><?CDATA ${H_{{\text{C}}1}},{\text{ }}{H_{{\text{C}}2}},{\text{ }}{H_{\text{P}}}$?></tex-math><mml:math overflow="scroll"><mml:mrow><mml:mrow><mml:msub><mml:mi>H</mml:mi><mml:mrow><mml:mrow><mml:mtext>C</mml:mtext></mml:mrow><mml:mn>1</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mo>,</mml:mo><mml:mrow><mml:mtext> </mml:mtext></mml:mrow><mml:mrow><mml:msub><mml:mi>H</mml:mi><mml:mrow><mml:mrow><mml:mtext>C</mml:mtext></mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mo>,</mml:mo><mml:mrow><mml:mtext> </mml:mtext></mml:mrow><mml:mrow><mml:msub><mml:mi>H</mml:mi><mml:mrow><mml:mtext>P</mml:mtext></mml:mrow></mml:msub></mml:mrow></mml:mrow></mml:math><inline-graphic xlink:href="https://content.cld.iop.org/journals/0953-2048/38/3/035028/revision2/sustadb6d8ieqn3.gif"/></inline-formula> and <inline-formula>
<tex-math><?CDATA ${H_{{\text{irr}}}}$?></tex-math><mml:math overflow="scroll"><mml:mrow><mml:mrow><mml:msub><mml:mi>H</mml:mi><mml:mrow><mml:mrow><mml:mtext>irr</mml:mtext></mml:mrow></mml:mrow></mml:msub></mml:mrow></mml:mrow></mml:math><inline-graphic xlink:href="https://content.cld.iop.org/journals/0953-2048/38/3/035028/revision2/sustadb6d8ieqn4.gif"/></inline-formula> were estimated and a vortex matter diagram was sketched. By using the Bean model, the critical current density values <inline-formula>
<tex-math><?CDATA ${J_{\text{C}}}\left( {T,H} \right)$?></tex-math><mml:math overflow="scroll"><mml:mrow><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:mtext>C</mml:mtext></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi>T</mml:mi><mml:mo>,</mml:mo><mml:mi>H</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:math><inline-graphic xlink:href="https://content.cld.iop.org/journals/0953-2048/38/3/035028/revision2/sustadb6d8ieqn5.gif"/></inline-formula> were obtained and the typical peak effect is observed. The vortex dynamics mechanism is discussed taking into account four vortex feature regimes in the double-logarithmical <inline-formula>
<tex-math><?CDATA ${J_{\text{C}}}\left( H \right)$?></tex-math><mml:math overflow="scroll"><mml:mrow><mml:mrow><mml:msub><mml:mi>J</mml:mi><mml:mrow><mml:mtext>C</mml:mtext></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mi>H</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:math><inline-graphic xlink:href="https://content.cld.iop.org/journals/0953-2048/38/3/035028/revision2/sustadb6d8ieqn6.gif"/></inline-formula> curves. The vortex pinning mechanism is discussed by obtaining the pining force, <inline-formula>
<tex-math><?CDATA ${F_{\text{P}}}$?></tex-math><mml:math overflow="scroll"><mml:mrow><mml:mrow><mml:msub><mml:mi>F</mml:mi><mml:mrow><mml:mtext>P</mml:mtext></mml:mrow></mml:msub></mml:mrow></mml:mrow></mml:math><inline-graphic xlink:href="https://content.cld.iop.org/journals/0953-2048/38/3/035028/revision2/sustadb6d8ieqn7.gif"/></inline-formula>, its normalization, <inline-formula>
<tex-math><?CDATA $f\left( h \right)$?></tex-math><mml:math overflow="scroll"><mml:mrow><mml:mi>f</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>h</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:math><inline-graphic xlink:href="https://content.cld.iop.org/journals/0953-2048/38/3/035028/revision2/sustadb6d8ieqn8.gif"/></inline-formula>, and magnetic relaxation <inline-formula>
<tex-math><?CDATA $M\left( t \right)$?></tex-math><mml:math overflow="scroll"><mml:mrow><mml:mi>M</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:math><inline-graphic xlink:href="https://content.cld.iop.org/journals/0953-2048/38/3/035028/revision2/sustadb6d8ieqn9.gif"/></inline-formula> measurements taken in field cooling mode at 10–60 K. The glassy exponent <inline-formula>
<tex-math><?CDATA $\mu $?></tex-math><mml:math overflow="scroll"><mml:mrow><mml:mi>μ</mml:mi></mml:mrow></mml:math><inline-graphic xlink:href="https://content.cld.iop.org/journals/0953-2048/38/3/035028/revision2/sustadb6d8ieqn10.gif"/></inline-formula> and the characteristic energy <inline-formula>
<tex-math><?CDATA $U\left( {J,{\text{ }}T} \right)$?></tex-math><mml:math overflow="scroll"><mml:mrow><mml:mi>U</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi>J</mml:mi><mml:mo>,</mml:mo><mml:mrow><mml:mtext> </mml:mtext></mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:math><inline-graphic xlink:href="https://content.cld.iop.org/journals/0953-2048/38/3/035028/revision2/sustadb6d8ieqn11.gif"/></inline-formula> in the vortex glass model were estimated following the Maley method. The collective-pinning model is used to discuss the possible vortex regimes mechanism (individual flux lines, small bundles and large bundles of pinned flux). Eventually, the <inline-formula>
<tex-math><?CDATA $E\left( J \right)$?></tex-math><mml:math overflow="scroll"><mml:mrow><mml:mi>E</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>J</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:math><inline-graphic xlink:href="https://content.cld.iop.org/journals/0953-2048/38/3/035028/revision2/sustadb6d8ieqn12.gif"/></inline-formula> curves, expressed from the swept field and creep measurements, show a power-law behaviour, in agreement with the vortex matter.</p></abstract><kwd-group kwd-group-type="author"><kwd>vortex dynamics</kwd><kwd>YBCO superconductor</kwd><kwd>uniaxial thin film</kwd><kwd>magnetic properties of YBCO</kwd></kwd-group><funding-group><award-group><funding-source>Peruvian Agency of Science CONCYTEC-PROCIENCIA</funding-source><award-id>E073-2023-01</award-id><award-id>PE501085381-2023-PROCIENCIA</award-id></award-group><award-group><funding-source>Universidade Federal de Pernambuco, Brazil</funding-source><award-id>13/2022</award-id><award-id>23076.101469/2021-69</award-id></award-group></funding-group><counts><page-count count="13"/></counts><custom-meta-group><custom-meta><meta-name>crossmark</meta-name><meta-value>yes</meta-value></custom-meta></custom-meta-group></article-meta></front><back><ack xmlns=""><title>Acknowledgments</title><p>This work has been supported by the Peruvian Agency of Science CONCYTEC-PROCIENCIA through Grant No. PE501085381-2023-PROCIENCIA entitled ‘Tesis de Pregrado y Posgrado en Ciencia, Tecnología e Innovación Tecnológica—Concurso E073-2023-01’. The work in UK has been supported by the Cambridge Royce facilities grant CAM-YR8-UI-009-REAS. The work in Brazil has been supported by the PROFESSOR VISITANTE Program No. 13/2022 of the Universidade Federal de Pernambuco, Brazil, Contract No. 019063/2023-39. A Aguiar thanks CNPQ, Brazil for supporting his research project.</p></ack></back></article>