<?xml version="1.0" encoding="utf-8"?>
<export-example>
  <doc>
    <id>27778</id>
    <completedYear/>
    <publishedYear>2021</publishedYear>
    <thesisYearAccepted/>
    <language>eng</language>
    <pageFirst>1506</pageFirst>
    <pageLast>1510</pageLast>
    <pageNumber/>
    <edition/>
    <issue>6562</issue>
    <volume>373</volume>
    <type>articler</type>
    <publisherName/>
    <publisherPlace/>
    <creatingCorporation/>
    <contributingCorporation/>
    <belongsToBibliography>0</belongsToBibliography>
    <completedDate>2021-09-24</completedDate>
    <publishedDate>--</publishedDate>
    <thesisDateAccepted>--</thesisDateAccepted>
    <title language="eng">Restored strange metal phase through suppression of charge density waves in underdoped YBa2Cu3O7–δ</title>
    <abstract language="eng">The normal state of optimally doped cuprates is dominated by the “strange metal” phase that shows a linear temperature (T) dependence of the resistivity persisting down to the lowest T. For underdoped cuprates, this behavior is lost below the pseudogap temperature T*, where charge density waves (CDWs), together with other intertwined local orders, characterize the ground state. We found that the T-linear resistivity of highly strained, ultrathin, underdoped YBa2Cu3O7–δ films is restored when the CDW amplitude, detected by resonant inelastic x-ray scattering, is suppressed. This observation suggests an intimate connection between the onset of CDWs and the departure from T-linear resistivity in underdoped cuprates. Our results illustrate the potential of using strain control to manipulate the ground state of quantum materials.</abstract>
    <parentTitle language="eng">Science</parentTitle>
    <identifier type="doi">10.1126/science.abc8372</identifier>
    <identifier type="url">https://www.science.org/doi/10.1126/science.abc8372</identifier>
    <enrichment key="BTU">an der BTU erstellt / created at BTU</enrichment>
    <enrichment key="opus.source">publish</enrichment>
    <enrichment key="Fprofil">1 Energiewende und Dekarbonisierung / Energy Transition and Decarbonisation</enrichment>
    <enrichment key="Fprofil">4 Künstliche Intelligenz und Sensorik / Artificial Intelligence and Sensor Technology</enrichment>
    <author>
      <firstName>Eric</firstName>
      <lastName>Wahlberg</lastName>
    </author>
    <submitter>
      <firstName>Katrin</firstName>
      <lastName>Gregor</lastName>
    </submitter>
    <author>
      <firstName>Riccardo</firstName>
      <lastName>Arpaia</lastName>
    </author>
    <author>
      <firstName>Götz</firstName>
      <lastName>Seibold</lastName>
    </author>
    <author>
      <firstName>Matteo</firstName>
      <lastName>Rossi</lastName>
    </author>
    <author>
      <firstName>Roberto</firstName>
      <lastName>Fumagalli</lastName>
    </author>
    <author>
      <firstName>Edoardo</firstName>
      <lastName>Trabaldo</lastName>
    </author>
    <author>
      <firstName>Nicholas B.</firstName>
      <lastName>Brookes</lastName>
    </author>
    <author>
      <firstName>Lucio</firstName>
      <lastName>Braicovich</lastName>
    </author>
    <author>
      <firstName>Sergio</firstName>
      <lastName>Caprara</lastName>
    </author>
    <author>
      <firstName>Floriana</firstName>
      <lastName>Lombardi</lastName>
    </author>
    <author>
      <firstName>Ulf</firstName>
      <lastName>Gran</lastName>
    </author>
    <author>
      <firstName>Giacomo Claudio</firstName>
      <lastName>Ghiringhelli</lastName>
    </author>
    <author>
      <firstName>Thilo</firstName>
      <lastName>Bauch</lastName>
    </author>
    <subject>
      <language>eng</language>
      <type>uncontrolled</type>
      <value>Cuprate superconductors</value>
    </subject>
    <subject>
      <language>eng</language>
      <type>uncontrolled</type>
      <value>Charge-Density Wave</value>
    </subject>
    <collection role="institutes" number="1501">FG Computational Physics</collection>
  </doc>
</export-example>
