{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.30953.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/176647"}},{"@id":"https://doi.org/10.1016/0370-2693(82)90325-2","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"UA5 Collaboration"},"creator":{"@type":"Organization","name":"UA5 Collaboration"},"datePublished":"1982","description":"CERN-ISR. P AP COLLISIONS AT SQRT(S) = 53 GEV OBSERVED IN THE UA5 STREAMER CHAMBER.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.30953.v1/t1","@type":"Dataset","description":"No description provided.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.30953.v1/t2","@type":"Dataset","description":"MOMENTS OF MULTIPLICITY DISTRIBUTIONS FOR P P AND P AP. MULT(NAME=DQ) IS &lt;(N-&lt;N&gt;)**Q&gt;**1/Q. MULT(NAME=NQ) IS .","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.30953.v1/t3","@type":"Dataset","description":"Data read from plot.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.30953.v1/t4","@type":"Dataset","description":"Data read from plot.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.30953.v1/t5","@type":"Dataset","description":"RATIO OF PSEUDORAPIDITY DENSITIES FROM P AP AND P P INTERACTIONS AS A FUNCTION OF ETARAP.","name":"Table 5"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins176647?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/30953"}],"inLanguage":"en","name":"Comparison of $p \\bar{p}$ and $p p$ Interactions at $\\sqrt{s}=53$-{GeV}","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins176647?version=1","version":1}
