{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.130268.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1783943"}},{"@id":"https://doi.org/10.1007/JHEP07(2020)016","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"LHCf Collaboration"},"creator":{"@type":"Organization","name":"LHCf Collaboration"},"datePublished":"2022","description":"Measurement of the energy flow, the cross section and the average inelasticity of forward neutrons (+ antineutrons) produced in $\\mathrm{\\sqrt{s} = 13\\,TeV}$ proton-proton collisions. These quantities are derived from the inclusive differential production cross section measured, as a function of energy, in the six pseudorapidity regions corresponding to $\\eta > 10.75$, $10.06 < \\eta < 10.75$, $9.65 < \\eta < 10.06$, $8.99 < \\eta < 9.21$, $8.80 < \\eta < 8.99$ and $8.65 < \\eta < 8.80$. The measurements refer to all neutrons (and antineutrons) directly produced in the collisions or resulting from the decay of short life particles ($\\mathrm{c \\tau<1\\,cm}$).","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.130268.v1/t1","@type":"Dataset","description":"Neutron (and antineutron) inclusive differential production cross section in $\\eta > 10.75$","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.130268.v1/t2","@type":"Dataset","description":"Neutron (and antineutron) inclusive differential production cross section in $10.06 < \\eta < 10.75$","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.130268.v1/t3","@type":"Dataset","description":"Neutron (and antineutron) inclusive differential production cross section in $9.65 < \\eta < 10.06$","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.130268.v1/t4","@type":"Dataset","description":"Neutron (and antineutron) inclusive differential production cross section in $8.99 < \\eta < 9.21$","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.130268.v1/t5","@type":"Dataset","description":"Neutron (and antineutron) inclusive differential production cross section in $8.80 < \\eta < 8.99$","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.130268.v1/t6","@type":"Dataset","description":"Neutron (and antineutron) inclusive differential production cross section in $8.65 < \\eta < 8.80$","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.130268.v1/t7","@type":"Dataset","description":"Neutron (and antineutron) inclusive differential energy flow vs pseudorapidity","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.130268.v1/t8","@type":"Dataset","description":"Neutron (and antineutron) inclusive differential production cross section vs pseudorapidity","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.130268.v1/t9","@type":"Dataset","description":"Neutron (and antineutron) inclusive production cross section vs elasticity","name":"Table 9"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1783943?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/130268"}],"inLanguage":"en","name":"Measurement of energy flow, cross section and average inelasticity of forward neutrons produced in $\\mathrm{\\sqrt{s} = 13 TeV}$ proton-proton collisions with the LHCf Arm2 detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1783943?version=1","version":1}