{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.41901.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/655225"}},{"@id":"https://doi.org/10.1016/j.physletb.2004.11.068","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"KLOE Collaboration"},"creator":{"@type":"Organization","name":"KLOE Collaboration"},"datePublished":"2005","description":"FRASCATI-DAPHNE. Measurement of the cross section for the process E+ E- --& gt; PI+ PI- GAMMA at a centre-of-mass energy of 1.02 GeV. The cross section for the E+ E- --& gt; PI+ PI- process is extracted from the dependence on the invariant mass of the two-pion system. The form factor is also calculated.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.41901.v1/t1","@type":"Dataset","description":"The differential cross section as a function of the invariant mass of the di-pion system in the angular region THETA(PIPI)...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.41901.v1/t2","@type":"Dataset","description":"The physical cross section for E+ E- --> PI+ PI- including FSR and vacuum polarization effects.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.41901.v1/t3","@type":"Dataset","description":"The pion form factor with FSR and vacuum polarization effects removed.","name":"Table 3"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins655225?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/41901"}],"inLanguage":"en","name":"Measurement of sigma(e+ e- --> pi+ pi- gamma) and extraction of sigma(e+ e- --> pi+ pi-) below 1-GeV with the KLOE detector.","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins655225?version=1","version":1}