Ontology type: schema:ScholarlyArticle Open Access: True
2019-12
AUTHORSCiarán Hickey, Simon Trebst
ABSTRACTIn the field of quantum magnetism, the exactly solvable Kitaev honeycomb model serves as a paradigm for the fractionalization of spin degrees of freedom and the formation of [Formula: see text] quantum spin liquids. An intense experimental search has led to the discovery of a number of spin-orbit entangled Mott insulators that realize its characteristic bond-directional interactions and, in the presence of magnetic fields, exhibit no indications of long-range order. Here, we map out the complete phase diagram of the Kitaev model in tilted magnetic fields and report the emergence of a distinct gapless quantum spin liquid at intermediate field strengths. Analyzing a number of static, dynamical, and finite temperature quantities using numerical exact diagonalization techniques, we find strong evidence that this phase exhibits gapless fermions coupled to a massless U(1) gauge field. We discuss its stability in the presence of perturbations that naturally arise in spin-orbit entangled candidate materials. More... »
PAGES530
http://scigraph.springernature.com/pub.10.1038/s41467-019-08459-9
DOIhttp://dx.doi.org/10.1038/s41467-019-08459-9
DIMENSIONShttps://app.dimensions.ai/details/publication/pub.1111779764
PUBMEDhttps://www.ncbi.nlm.nih.gov/pubmed/30705263
JSON-LD is the canonical representation for SciGraph data.
TIP: You can open this SciGraph record using an external JSON-LD service: JSON-LD Playground Google SDTT
[
{
"@context": "https://springernature.github.io/scigraph/jsonld/sgcontext.json",
"about": [
{
"id": "http://purl.org/au-research/vocabulary/anzsrc-for/2008/0202",
"inDefinedTermSet": "http://purl.org/au-research/vocabulary/anzsrc-for/2008/",
"name": "Atomic, Molecular, Nuclear, Particle and Plasma Physics",
"type": "DefinedTerm"
},
{
"id": "http://purl.org/au-research/vocabulary/anzsrc-for/2008/02",
"inDefinedTermSet": "http://purl.org/au-research/vocabulary/anzsrc-for/2008/",
"name": "Physical Sciences",
"type": "DefinedTerm"
}
],
"author": [
{
"affiliation": {
"alternateName": "University of Cologne",
"id": "https://www.grid.ac/institutes/grid.6190.e",
"name": [
"Institute for Theoretical Physics, University of Cologne, 50937, Cologne, Germany"
],
"type": "Organization"
},
"familyName": "Hickey",
"givenName": "Ciar\u00e1n",
"type": "Person"
},
{
"affiliation": {
"alternateName": "University of Cologne",
"id": "https://www.grid.ac/institutes/grid.6190.e",
"name": [
"Institute for Theoretical Physics, University of Cologne, 50937, Cologne, Germany"
],
"type": "Organization"
},
"familyName": "Trebst",
"givenName": "Simon",
"type": "Person"
}
],
"citation": [
{
"id": "https://doi.org/10.1103/physrevlett.110.097204",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1001186415"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.110.097204",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1001186415"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1088/0034-4885/80/1/016502",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1002855287"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.91.180401",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1006986407"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.91.180401",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1006986407"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.84.125125",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1007074128"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.84.125125",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1007074128"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.89.085121",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1007704629"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.89.085121",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1007704629"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.85.235151",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1009895404"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.85.235151",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1009895404"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.112.207203",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1010777408"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.112.207203",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1010777408"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1016/0025-5408(73)90167-0",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1012450990"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1016/0025-5408(73)90167-0",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1012450990"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.86.075115",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1016097803"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.86.075115",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1016097803"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.62.7850",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1016637347"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.62.7850",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1016637347"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1016/0550-3213(77)90086-4",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1017221832"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1016/0550-3213(77)90086-4",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1017221832"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.112.077204",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1023253702"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.112.077204",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1023253702"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.105.027204",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1023419687"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.105.027204",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1023419687"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.69.2142",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1023753456"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.69.2142",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1023753456"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.84.085141",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1023791923"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.84.085141",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1023791923"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1016/j.aop.2005.10.005",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1025107810"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.102.017205",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1026932870"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.102.017205",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1026932870"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.83.245104",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1028929352"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.83.245104",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1028929352"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.111.010401",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1034599000"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.111.010401",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1034599000"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1146/annurev-conmatphys-031115-011319",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1037858925"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.91.094422",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1040867753"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.91.094422",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1040867753"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.99.266403",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1045152286"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.99.266403",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1045152286"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.113.197205",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1046335625"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.113.197205",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1046335625"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevx.5.041035",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1048363728"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevx.5.041035",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1048363728"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.108.240401",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1049308442"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.108.240401",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1049308442"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.91.115111",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1052428141"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.91.115111",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1052428141"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.84.180407",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1060637322"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.84.180407",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1060637322"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.92.115127",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1060647080"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.92.115127",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1060647080"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.92.235119",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1060648185"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.92.235119",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1060648185"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.93.085101",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1060649134"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.93.085101",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1060649134"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.66.1773",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1060802261"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.66.1773",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1060802261"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1142/s0217984991000058",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1062947462"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1143/ptps.160.155",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1063143620"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.95.180411",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1085784082"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.95.180411",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1085784082"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.95.241112",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1090221055"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.95.241112",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1090221055"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.96.064430",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1091357784"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.96.064430",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1091357784"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1146/annurev-conmatphys-033117-053934",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1092329976"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1137/1.9780898719628",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1098556223"
],
"type": "CreativeWork"
},
{
"id": "sg:pub.10.1038/s41535-018-0079-2",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1100951705",
"https://doi.org/10.1038/s41535-018-0079-2"
],
"type": "CreativeWork"
},
{
"id": "sg:pub.10.1038/s41535-018-0079-2",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1100951705",
"https://doi.org/10.1038/s41535-018-0079-2"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physicsphysiquefizika.2.5",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1101010436"
],
"type": "CreativeWork"
},
{
"id": "sg:pub.10.1038/s41567-018-0129-5",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1103817430",
"https://doi.org/10.1038/s41567-018-0129-5"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.120.217205",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1104244482"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.120.217205",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1104244482"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.97.241110",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1104689078"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.97.241110",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1104689078"
],
"type": "CreativeWork"
},
{
"id": "sg:pub.10.1038/s41586-018-0274-0",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1105348580",
"https://doi.org/10.1038/s41586-018-0274-0"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.98.014418",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1105672528"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.98.014418",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1105672528"
],
"type": "CreativeWork"
}
],
"datePublished": "2019-12",
"datePublishedReg": "2019-12-01",
"description": "In the field of quantum magnetism, the exactly solvable Kitaev honeycomb model serves as a paradigm for the fractionalization of spin degrees of freedom and the formation of [Formula: see text] quantum spin liquids. An intense experimental search has led to the discovery of a number of spin-orbit entangled Mott insulators that realize its characteristic bond-directional interactions and, in the presence of magnetic fields, exhibit no indications of long-range order. Here, we map out the complete phase diagram of the Kitaev model in tilted magnetic fields and report the emergence of a distinct gapless quantum spin liquid at intermediate field strengths. Analyzing a number of static, dynamical, and finite temperature quantities using numerical exact diagonalization techniques, we find strong evidence that this phase exhibits gapless fermions coupled to a massless U(1) gauge field. We discuss its stability in the presence of perturbations that naturally arise in spin-orbit entangled candidate materials.",
"genre": "research_article",
"id": "sg:pub.10.1038/s41467-019-08459-9",
"inLanguage": [
"en"
],
"isAccessibleForFree": true,
"isPartOf": [
{
"id": "sg:journal.1043282",
"issn": [
"2041-1723"
],
"name": "Nature Communications",
"type": "Periodical"
},
{
"issueNumber": "1",
"type": "PublicationIssue"
},
{
"type": "PublicationVolume",
"volumeNumber": "10"
}
],
"name": "Emergence of a field-driven U(1) spin liquid in the Kitaev honeycomb model",
"pagination": "530",
"productId": [
{
"name": "readcube_id",
"type": "PropertyValue",
"value": [
"e58afc2cd0f42928677186e94ce7d451d3f97d7a56bc6ffd86eb543b0a261786"
]
},
{
"name": "pubmed_id",
"type": "PropertyValue",
"value": [
"30705263"
]
},
{
"name": "nlm_unique_id",
"type": "PropertyValue",
"value": [
"101528555"
]
},
{
"name": "doi",
"type": "PropertyValue",
"value": [
"10.1038/s41467-019-08459-9"
]
},
{
"name": "dimensions_id",
"type": "PropertyValue",
"value": [
"pub.1111779764"
]
}
],
"sameAs": [
"https://doi.org/10.1038/s41467-019-08459-9",
"https://app.dimensions.ai/details/publication/pub.1111779764"
],
"sdDataset": "articles",
"sdDatePublished": "2019-04-11T12:52",
"sdLicense": "https://scigraph.springernature.com/explorer/license/",
"sdPublisher": {
"name": "Springer Nature - SN SciGraph project",
"type": "Organization"
},
"sdSource": "s3://com-uberresearch-data-dimensions-target-20181106-alternative/cleanup/v134/2549eaecd7973599484d7c17b260dba0a4ecb94b/merge/v9/a6c9fde33151104705d4d7ff012ea9563521a3ce/jats-lookup/v90/0000000364_0000000364/records_72836_00000001.jsonl",
"type": "ScholarlyArticle",
"url": "https://www.nature.com/articles/s41467-019-08459-9"
}
]
Download the RDF metadata as: json-ld nt turtle xml License info
JSON-LD is a popular format for linked data which is fully compatible with JSON.
curl -H 'Accept: application/ld+json' 'https://scigraph.springernature.com/pub.10.1038/s41467-019-08459-9'
N-Triples is a line-based linked data format ideal for batch operations.
curl -H 'Accept: application/n-triples' 'https://scigraph.springernature.com/pub.10.1038/s41467-019-08459-9'
Turtle is a human-readable linked data format.
curl -H 'Accept: text/turtle' 'https://scigraph.springernature.com/pub.10.1038/s41467-019-08459-9'
RDF/XML is a standard XML format for linked data.
curl -H 'Accept: application/rdf+xml' 'https://scigraph.springernature.com/pub.10.1038/s41467-019-08459-9'
This table displays all metadata directly associated to this object as RDF triples.
211 TRIPLES
21 PREDICATES
74 URIs
21 LITERALS
9 BLANK NODES