{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.91963.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1747892"}},{"@id":"https://doi.org/10.1140/epjc/s10052-019-7402-3","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2021","description":"The average total energy as well as its hadronic and electromagnetic components are measured with the CMS detector at pseudorapidities \u22126.6&lt;eta&lt;\u22125.2 in proton-proton collisions at a centre-of-mass energy sqrt(s)=13 TeV. The results are presented as a function of the charged particle multiplicity in the region |\u03b7|&lt;2. This measurement is sensitive to correlations induced by the underlying event structure over a very wide pseudorapidity region. The predictions of Monte Carlo event generators commonly used in collider experiments and ultra-high energy cosmic ray physics are compared to the data.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.91963.v1/t1","@type":"Dataset","description":"Average total energy reconstructed in the region \u22126.6 &lt; eta &lt; \u22125.2 as a function of the number of reconstructed...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.91963.v1/t2","@type":"Dataset","description":"Average total energiy reconstructed in the region \u22126.6 &lt; eta &lt; \u22125.2 normalised to that in the first bin (Nch&lt;...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.91963.v1/t3","@type":"Dataset","description":"Average electromagnetic energy reconstructed in the region \u22126.6 &lt; eta &lt; \u22125.2 as a function of the number of reconstructed...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.91963.v1/t4","@type":"Dataset","description":"Average hadronic energy reconstructed in the region \u22126.6 &lt; eta &lt; \u22125.2 as a function of the number of reconstructed...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.91963.v1/t5","@type":"Dataset","description":"Ratio of the average electromagnetic and hadronic energies reconstructed in the region \u22126.6 &lt; eta &lt; \u22125.2 as a function...","name":"Table 5"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1747892?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/91963"}],"inLanguage":"en","name":"Measurement of the average very forward energy as a function of the track multiplicity at central pseudorapidities in proton-proton collisions at $\\sqrt{s} =$ 13 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1747892?version=1","version":1}
