{"data":{"id":"10.15151/esrf-es-1734554406","type":"dois","attributes":{"doi":"10.15151/esrf-es-1734554406","prefix":"10.15151","suffix":"esrf-es-1734554406","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Chen, Wei Tin","nameType":"Personal","givenName":"Wei Tin","familyName":"Chen","affiliation":["National Taiwan University,Center for Condensed Matter Sciences,1 Roosevelt Rd,Section 4,106 TAIPEI,106,TAIPEI,TAIWAN"],"nameIdentifiers":[{"schemeUri":"https://orcid.org","nameIdentifier":"https://orcid.org/0000-0003-4007-2984","nameIdentifierScheme":"ORCID"}]},{"name":"Ladbrook, Evangeline","nameType":"Personal","givenName":"Evangeline","familyName":"Ladbrook","affiliation":["University of Warwick,Department of Chemistry,West Midlands,CV4 7AL COVENTRY,UNITED KINGDOM,CV4 7AL,COVENTRY,UNITED KINGDOM"],"nameIdentifiers":[]},{"name":"Senn, Mark Stephen","nameType":"Personal","givenName":"Mark Stephen","familyName":"Senn","affiliation":["University of Warwick,Department of Chemistry,West Midlands,CV4 7AL COVENTRY,UNITED KINGDOM,CV4 7AL,COVENTRY,UNITED KINGDOM"],"nameIdentifiers":[{"schemeUri":"https://orcid.org","nameIdentifier":"https://orcid.org/0000-0003-0812-5281","nameIdentifierScheme":"ORCID"}]},{"name":"Simpson, Struan","nameType":"Personal","givenName":"Struan","familyName":"Simpson","affiliation":["University of Warwick,Department of Chemistry,West Midlands,CV4 7AL COVENTRY,UNITED KINGDOM,CV4 7AL,COVENTRY,UNITED KINGDOM"],"nameIdentifiers":[]}],"titles":[{"title":"Mapping the structural domains associated with the suppression of the 3D superconducting state in the high-Tc layered cuprate"}],"publisher":"European Synchrotron Radiation Facility","container":{},"publicationYear":2027,"subjects":[{"subject":"Hard Condensed Matter Science","subjectScheme":"Proposal Type Description"},{"subject":"HC-5590","subjectScheme":"Proposal"},{"subject":"ID11","subjectScheme":"Instrument"},{"subject":"x-ray probe","valueUri":"http://purl.org/pan-science/PaNET/PaNET01012","schemeUri":"http://purl.org/pan-science/PaNET/PaNET.owl","subjectScheme":"PaNET","classificationCode":"PaNET01012"}],"contributors":[{"name":"Wright, Jonathan","nameType":"Personal","givenName":"Jonathan","familyName":"Wright","affiliation":["ESRF,CS 40220,38043 GRENOBLE Cedex 9,FRANCE,38043,GRENOBLE,FRANCE"],"contributorType":"DataCollector","nameIdentifiers":[{"schemeUri":"https://orcid.org","nameIdentifier":"https://orcid.org/0000-0002-8217-0884","nameIdentifierScheme":"ORCID"}]}],"dates":[{"date":"2024-07-19","dateType":"Collected"},{"date":"2027","dateType":"Issued"}],"language":"en","types":{"ris":"DATA","bibtex":"misc","citeproc":"dataset","schemaOrg":"Dataset","resourceType":"Experiment Session","resourceTypeGeneral":"Dataset"},"relatedIdentifiers":[],"relatedItems":[],"sizes":[],"formats":[],"version":null,"rightsList":[],"descriptions":[{"description":"Competition exists in the high temperature cuprate superconductors between the superconducting (SC), pseudogap and ordered charge density wave (CDW)\r\nstates. A key doping level for understanding these competitions has been the 1/8 doping level, where an anomaly in the superconducting dome occurs (e.g., La2- xBaxCuO4), that is concomitant with a first order structural phase transition and is understood to supress 3D superconductivity. However, very recently we have shown that this structural phase transition does not run to completion, suggesting a natural explanation for the persistence of only 2D (in plane) SC at the 1/8 anomaly. We propose to carry out a diffraction resolved tomography experiment on a surrogate system to map out how the structural domains associated with the suppression of the 3D superconducting state percolate.","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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