{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.44998.v2","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/395196"}},{"@id":"https://doi.org/10.1007/BF01579802","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ZEUS Collaboration"},"creator":{"@type":"Organization","name":"ZEUS Collaboration"},"datePublished":"2021","description":"DESY-HERA. ZEUS Collaboration. Measurements of K0 and Lambda production in neutral current deep inelastic scattering of 26.7 GeV electrons and 820 GeV protons in the kinematic range Q**2 from 10 to 640 GeV**2, x from 0.0003 to 0.01 and Jacquet-Blondel rapidity & gt; 0.04. Data for differential multiplicity distributions requested from the authors.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.44998.v2/t1","@type":"Dataset","description":"No description provided.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.44998.v2/t2","@type":"Dataset","description":"No description provided.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.44998.v2/t3","@type":"Dataset","description":"No description provided.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.44998.v2/t4","@type":"Dataset","description":"No description provided.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.44998.v2/t5","@type":"Dataset","description":"Mean K0 multiplicity as a function of Q**2.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.44998.v2/t6","@type":"Dataset","description":"Ratio of mean K0 multiplicity to mean charged particle multiplicity.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.44998.v2/t7","@type":"Dataset","description":"Differential K0 multiplicity in non-rapidity gap (NRG) data.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.44998.v2/t8","@type":"Dataset","description":"Differential K0 multiplicity in large-rapidity gap (LRG) data.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.44998.v2/t9","@type":"Dataset","description":"Differential K0 multiplicity in non-rapidity gap (NRG) data.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.44998.v2/t10","@type":"Dataset","description":"Differential K0 multiplicity in large-rapidity gap (LRG) data.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.44998.v2/t11","@type":"Dataset","description":"No description provided.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.44998.v2/t12","@type":"Dataset","description":"No description provided.","name":"Table 12"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins395196?version=2"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/44998"}],"inLanguage":"en","name":"Neutral strange particle production in deep inelastic scattering at HERA","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins395196?version=2","version":2}