{"data":{"id":"10.4121/4de9f6fe-261e-43b7-aa73-69f79f3d7c6b","type":"dois","attributes":{"doi":"10.4121/4de9f6fe-261e-43b7-aa73-69f79f3d7c6b","prefix":"10.4121","suffix":"4de9f6fe-261e-43b7-aa73-69f79f3d7c6b","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"La Rivière, Bowy","nameType":"Personal","givenName":"Bowy","familyName":"La Rivière","nameIdentifiers":[{"nameIdentifier":"0009-0007-6373-0595","nameIdentifierScheme":"https://orcid.org/"}],"affiliation":[]},{"name":"Chepiga, Natalia","nameType":"Personal","givenName":"Natalia","familyName":"Chepiga","nameIdentifiers":[{"nameIdentifier":"0000-0002-5313-5035","nameIdentifierScheme":"https://orcid.org/"}],"affiliation":[]}],"titles":[{"title":"Data and processing tools supporting results presented in publication \"Z4 transitions in quantum loop models on a zig-zag ladder\" and chapter 6 in PhD thesis \"quantum criticality in frustrated Haldane chains and (doped) quantum loop models\""}],"publisher":"4TU.ResearchData","container":{},"publicationYear":2026,"subjects":[{"subject":"Condensed Matter Physics","subjectScheme":"Australian and New Zealand Standard Research Classification (ANZSRC), 2008","classificationCode":"0204"},{"subject":"FOS: Physical sciences","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"Quantum Physics","subjectScheme":"Australian and New Zealand Standard Research Classification (ANZSRC), 2008","classificationCode":"0206"},{"subject":"Physical Sciences","subjectScheme":"Australian and New Zealand Standard Research Classification (ANZSRC), 2008","classificationCode":"02"},{"subject":"density matrix renormalization group"},{"subject":"quantum magnetism"},{"subject":"exotic phases of matter"},{"subject":"quantum phase transitions"},{"subject":"quantum criticality"},{"subject":"quantum dimer and loop models"}],"contributors":[{"name":"Kavli Institute of Nanoscience, Delft University of Technology","nameType":"Organizational","affiliation":[],"contributorType":"Other","nameIdentifiers":[]}],"dates":[{"date":"2026-05-11","dateType":"Issued"}],"language":"en","types":{"ris":"DATA","bibtex":"misc","citeproc":"dataset","schemaOrg":"Dataset","resourceType":"Dataset","resourceTypeGeneral":"Dataset"},"relatedIdentifiers":[{"relationType":"IsSupplementTo","relatedIdentifier":"10.21468/scipostphys.17.5.144","relatedIdentifierType":"DOI"},{"relationType":"IsVersionOf","relatedIdentifier":"10.4121/4de9f6fe-261e-43b7-aa73-69f79f3d7c6b.v1","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":[],"formats":[".jld2, .jl"],"version":"1","rightsList":[{"rights":"Restrictive Licence","rightsUri":"https://data.4tu.nl/info/fileadmin/user_upload/Documenten/4TU.ResearchData_Restricted_Data_2022.pdf"}],"descriptions":[{"description":"This dataset includes data obtained from large-scale simulations performed with the density matrix renormalization group algorithm, and the tools used to process this data. 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This can be done to the point where the chiral transition turns into first order, we argue that this is associated with the emergence of a critical end 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