Ontology type: schema:ScholarlyArticle Open Access: True
2018-09
AUTHORSA. del Campo, J. Molina-Vilaplana, L. F. Santos, J. Sonner
ABSTRACTScrambling in interacting quantum systems out of equilibrium is particularly effective in the chaotic regime. Under time evolution, initially localized information is said to be scrambled as it spreads throughout the entire system. This spreading can be analyzed with the spectral form factor, which is defined in terms of the analytic continuation of the partition function. The latter is equivalent to the survival probability of a thermofield double state under unitary dynamics. Using random matrices from the Gaussian unitary ensemble (GUE) as Hamiltonians for the time evolution, we obtain exact analytical expressions at finite N for the survival probability. Numerical simulations of the survival probability with matrices taken from the Gaussian orthogonal ensemble (GOE) are also provided. The GOE is more suitable for our comparison with numerical results obtained with a disordered spin chain with local interactions. Common features between the random matrix and the realistic disordered model in the chaotic regime are identified. The differences that emerge as the spin model approaches a many-body localized phase are also discussed. More... »
PAGES247-258
http://scigraph.springernature.com/pub.10.1140/epjst/e2018-00083-5
DOIhttp://dx.doi.org/10.1140/epjst/e2018-00083-5
DIMENSIONShttps://app.dimensions.ai/details/publication/pub.1107296145
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/2008/0104",
"inDefinedTermSet": "http://purl.org/au-research/vocabulary/anzsrc-for/2008/",
"name": "Statistics",
"type": "DefinedTerm"
},
{
"id": "http://purl.org/au-research/vocabulary/anzsrc-for/2008/01",
"inDefinedTermSet": "http://purl.org/au-research/vocabulary/anzsrc-for/2008/",
"name": "Mathematical Sciences",
"type": "DefinedTerm"
}
],
"author": [
{
"affiliation": {
"alternateName": "University of Massachusetts Amherst",
"id": "https://www.grid.ac/institutes/grid.266683.f",
"name": [
"Department of Physics, University of Massachusetts, 02125, Boston, MA, USA"
],
"type": "Organization"
},
"familyName": "del Campo",
"givenName": "A.",
"id": "sg:person.01154611451.27",
"sameAs": [
"https://app.dimensions.ai/discover/publication?and_facet_researcher=ur.01154611451.27"
],
"type": "Person"
},
{
"affiliation": {
"alternateName": "Polytechnic University of Cartagena",
"id": "https://www.grid.ac/institutes/grid.218430.c",
"name": [
"Department of Systems Engineering, Technical University of Cartagena, C/Dr Fleming S/N, 30202, Cartagena, Spain"
],
"type": "Organization"
},
"familyName": "Molina-Vilaplana",
"givenName": "J.",
"id": "sg:person.012115476545.55",
"sameAs": [
"https://app.dimensions.ai/discover/publication?and_facet_researcher=ur.012115476545.55"
],
"type": "Person"
},
{
"affiliation": {
"alternateName": "Yeshiva University",
"id": "https://www.grid.ac/institutes/grid.268433.8",
"name": [
"Department of Physics, Yeshiva University, 10016, New York, NA, USA"
],
"type": "Organization"
},
"familyName": "Santos",
"givenName": "L. F.",
"id": "sg:person.0760461155.16",
"sameAs": [
"https://app.dimensions.ai/discover/publication?and_facet_researcher=ur.0760461155.16"
],
"type": "Person"
},
{
"affiliation": {
"alternateName": "University of Geneva",
"id": "https://www.grid.ac/institutes/grid.8591.5",
"name": [
"Department of Theoretical Physics, University of Geneva, 24 quai Ernest-Ansermet, 1211, Gen\u00e8ve 4, Switzerland"
],
"type": "Organization"
},
"familyName": "Sonner",
"givenName": "J.",
"id": "sg:person.01312202724.30",
"sameAs": [
"https://app.dimensions.ai/discover/publication?and_facet_researcher=ur.01312202724.30"
],
"type": "Person"
}
],
"citation": [
{
"id": "https://doi.org/10.1103/physreva.69.042304",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1001570458"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physreva.69.042304",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1001570458"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1088/0305-4470/37/17/004",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1003491686"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1002/prop.200410157",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1004245644"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1146/annurev-conmatphys-031214-014726",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1005301775"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physreve.89.062110",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1007455876"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physreve.89.062110",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1007455876"
],
"type": "CreativeWork"
},
{
"id": "sg:pub.10.1007/jhep05(2015)132",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1010538237",
"https://doi.org/10.1007/jhep05(2015)132"
],
"type": "CreativeWork"
},
{
"id": "sg:pub.10.1007/jhep05(2015)132",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1010538237",
"https://doi.org/10.1007/jhep05(2015)132"
],
"type": "CreativeWork"
},
{
"id": "sg:pub.10.1088/1126-6708/2008/10/065",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1013450009",
"https://doi.org/10.1088/1126-6708/2008/10/065"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1088/0031-8949/2015/t165/014018",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1015116263"
],
"type": "CreativeWork"
},
{
"id": "sg:pub.10.1038/nature13461",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1021784656",
"https://doi.org/10.1038/nature13461"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1016/s0370-1573(99)00083-6",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1022092215"
],
"type": "CreativeWork"
},
{
"id": "sg:pub.10.1088/1126-6708/2007/09/120",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1023220297",
"https://doi.org/10.1088/1126-6708/2007/09/120"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physreve.65.026214",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1027273502"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physreve.65.026214",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1027273502"
],
"type": "CreativeWork"
},
{
"id": "sg:pub.10.1007/jhep08(2016)106",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1027546612",
"https://doi.org/10.1007/jhep08(2016)106"
],
"type": "CreativeWork"
},
{
"id": "sg:pub.10.1007/jhep08(2016)106",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1027546612",
"https://doi.org/10.1007/jhep08(2016)106"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1088/0034-4885/41/4/003",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1027770822"
],
"type": "CreativeWork"
},
{
"id": "sg:pub.10.1088/1126-6708/2003/04/021",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1028201206",
"https://doi.org/10.1088/1126-6708/2003/04/021"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.92.014208",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1028243758"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.92.014208",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1028243758"
],
"type": "CreativeWork"
},
{
"id": "sg:pub.10.1007/bf01341708",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1029387957",
"https://doi.org/10.1007/bf01341708"
],
"type": "CreativeWork"
},
{
"id": "sg:pub.10.1088/1126-6708/2003/11/047",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1029796765",
"https://doi.org/10.1088/1126-6708/2003/11/047"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1016/0375-9601(77)90251-1",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1030652823"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1016/0375-9601(77)90251-1",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1030652823"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.115.211601",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1031640292"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.115.211601",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1031640292"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physreva.84.012113",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1033110366"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physreva.84.012113",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1033110366"
],
"type": "CreativeWork"
},
{
"id": "sg:pub.10.1038/nature13450",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1034207208",
"https://doi.org/10.1038/nature13450"
],
"type": "CreativeWork"
},
{
"id": "sg:pub.10.1140/epjd/e2009-00165-x",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1034297073",
"https://doi.org/10.1140/epjd/e2009-00165-x"
],
"type": "CreativeWork"
},
{
"id": "sg:pub.10.1007/978-3-642-03174-8_9",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1036507446",
"https://doi.org/10.1007/978-3-642-03174-8_9"
],
"type": "CreativeWork"
},
{
"id": "sg:pub.10.1007/978-3-642-03174-8_9",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1036507446",
"https://doi.org/10.1007/978-3-642-03174-8_9"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physreva.89.043620",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1038850231"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physreva.89.043620",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1038850231"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1088/1367-2630/16/6/063010",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1039278235"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1002/andp.201600284",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1039578213"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physreve.55.4067",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1041341043"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physreve.55.4067",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1041341043"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physreva.90.033623",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1041617128"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physreva.90.033623",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1041617128"
],
"type": "CreativeWork"
},
{
"id": "sg:pub.10.1007/jhep04(2013)022",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1042231337",
"https://doi.org/10.1007/jhep04(2013)022"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1016/j.cplett.2005.12.025",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1042641772"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1016/s0370-2693(98)00377-3",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1044092489"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevx.5.041025",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1047110770"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevx.5.041025",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1047110770"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.81.020405",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1053492603"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.81.020405",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1053492603"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1088/1367-2630/11/4/043026",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1059134649"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1088/1367-2630/11/4/043026",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1059134649"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1088/1367-2630/18/1/015014",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1059137086"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physreva.46.4650",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1060486285"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physreva.46.4650",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1060486285"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physreva.94.040302",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1060516755"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physreva.94.040302",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1060516755"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physreva.94.041603",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1060516761"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physreva.94.041603",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1060516761"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physreva.95.013604",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1060517497"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physreva.95.013604",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1060517497"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevd.16.520",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1060685429"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevd.16.520",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1060685429"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.56.2449",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1060793279"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.56.2449",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1060793279"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.84.2714",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1060820965"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.84.2714",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1060820965"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/revmodphys.53.385",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1060838979"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/revmodphys.53.385",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1060838979"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1126/science.1150841",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1062457162"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1126/science.aaa7432",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1062665386"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.4310/atmp.1998.v2.n2.a1",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1072456893"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.4310/atmp.1998.v2.n2.a2",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1072456894"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1002/andp.201600350",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1085411187"
],
"type": "CreativeWork"
},
{
"id": "sg:pub.10.1038/nphys4119",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1085463614",
"https://doi.org/10.1038/nphys4119"
],
"type": "CreativeWork"
},
{
"id": "sg:pub.10.1038/nphys4119",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1085463614",
"https://doi.org/10.1038/nphys4119"
],
"type": "CreativeWork"
},
{
"id": "sg:pub.10.1007/jhep05(2017)118",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1085559666",
"https://doi.org/10.1007/jhep05(2017)118"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1093/ptep/ptx108",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1090564080"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevx.7.031011",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1090809109"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevx.7.031011",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1090809109"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.119.040501",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1090959808"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.119.040501",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1090959808"
],
"type": "CreativeWork"
},
{
"id": "sg:pub.10.1007/jhep08(2017)075",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1091243246",
"https://doi.org/10.1007/jhep08(2017)075"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.119.130401",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1092017163"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.119.130401",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1092017163"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1098/rsta.2016.0434",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1092447777"
],
"type": "CreativeWork"
},
{
"id": "sg:pub.10.1007/jhep11(2017)048",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1092617685",
"https://doi.org/10.1007/jhep11(2017)048"
],
"type": "CreativeWork"
},
{
"id": "sg:pub.10.1007/jhep11(2017)149",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1092941371",
"https://doi.org/10.1007/jhep11(2017)149"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.120.070501",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1101010372"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevlett.120.070501",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1101010372"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.97.060303",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1101203127"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevb.97.060303",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1101203127"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevd.95.126008",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1101994616"
],
"type": "CreativeWork"
},
{
"id": "https://doi.org/10.1103/physrevd.95.126008",
"sameAs": [
"https://app.dimensions.ai/details/publication/pub.1101994616"
],
"type": "CreativeWork"
}
],
"datePublished": "2018-09",
"datePublishedReg": "2018-09-01",
"description": "Scrambling in interacting quantum systems out of equilibrium is particularly effective in the chaotic regime. Under time evolution, initially localized information is said to be scrambled as it spreads throughout the entire system. This spreading can be analyzed with the spectral form factor, which is defined in terms of the analytic continuation of the partition function. The latter is equivalent to the survival probability of a thermofield double state under unitary dynamics. Using random matrices from the Gaussian unitary ensemble (GUE) as Hamiltonians for the time evolution, we obtain exact analytical expressions at finite N for the survival probability. Numerical simulations of the survival probability with matrices taken from the Gaussian orthogonal ensemble (GOE) are also provided. The GOE is more suitable for our comparison with numerical results obtained with a disordered spin chain with local interactions. Common features between the random matrix and the realistic disordered model in the chaotic regime are identified. The differences that emerge as the spin model approaches a many-body localized phase are also discussed.",
"genre": "research_article",
"id": "sg:pub.10.1140/epjst/e2018-00083-5",
"inLanguage": [
"en"
],
"isAccessibleForFree": true,
"isPartOf": [
{
"id": "sg:journal.1297403",
"issn": [
"1951-6355",
"1951-6401"
],
"name": "The European Physical Journal Special Topics",
"type": "Periodical"
},
{
"issueNumber": "3-4",
"type": "PublicationIssue"
},
{
"type": "PublicationVolume",
"volumeNumber": "227"
}
],
"name": "Decay of a thermofield-double state in chaotic quantum systems",
"pagination": "247-258",
"productId": [
{
"name": "readcube_id",
"type": "PropertyValue",
"value": [
"1cccdbe7749294878524a52ed1bf8b773c777ab46bda2ffbac86deef314035fe"
]
},
{
"name": "doi",
"type": "PropertyValue",
"value": [
"10.1140/epjst/e2018-00083-5"
]
},
{
"name": "dimensions_id",
"type": "PropertyValue",
"value": [
"pub.1107296145"
]
}
],
"sameAs": [
"https://doi.org/10.1140/epjst/e2018-00083-5",
"https://app.dimensions.ai/details/publication/pub.1107296145"
],
"sdDataset": "articles",
"sdDatePublished": "2019-04-10T21:00",
"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/v90/0000000001_0000000264/records_8684_00000605.jsonl",
"type": "ScholarlyArticle",
"url": "https://link.springer.com/10.1140%2Fepjst%2Fe2018-00083-5"
}
]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.10.1140/epjst/e2018-00083-5'
N-Triples is a line-based linked data format ideal for batch operations.
curl -H 'Accept: application/n-triples' 'https://scigraph.springernature.com/pub.10.1140/epjst/e2018-00083-5'
Turtle is a human-readable linked data format.
curl -H 'Accept: text/turtle' 'https://scigraph.springernature.com/pub.10.1140/epjst/e2018-00083-5'
RDF/XML is a standard XML format for linked data.
curl -H 'Accept: application/rdf+xml' 'https://scigraph.springernature.com/pub.10.1140/epjst/e2018-00083-5'
This table displays all metadata directly associated to this object as RDF triples.
294 TRIPLES
21 PREDICATES
89 URIs
19 LITERALS
7 BLANK NODES