{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.89874.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1736730"}},{"@id":"https://doi.org/10.1103/PhysRevLett.124.031802","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2019","description":"A search for magnetic monopoles and high-electric-charge objects is presented using 34.4 fb$^{-1}$ of 13 TeV $pp$ collision data collected by the ATLAS detector at the LHC during 2015 and 2016. The considered signature is based upon high ionization in the transition radiation tracker of the inner detector associated with a pencil-shape energy deposit in the electromagnetic calorimeter. The data were collected by a dedicated trigger based on the tracker high-threshold hit capability. The results are interpreted in models of Drell-Yan pair production of stable particles with two spin hypotheses (0 and 1/2) and masses ranging from 200 GeV to 4000 GeV. The search improves by approximately a factor of five the constraints on the direct production of magnetic monopoles carrying one or two Dirac magnetic charges and stable objects with electric charge in the range $20\\le|z|\\le60$ and extends the charge range to $60<|z|\\le100$.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.89874.v1/t1","@type":"Dataset","description":"Observed 95% confidence-level upper limits on the cross section for Drell-Yan spin-0 monopole production as a function of mass for...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.89874.v1/t2","@type":"Dataset","description":"Observed 95% confidence-level upper limits on the cross section for Drell-Yan spin-0 HECO production as a function of mass for...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.89874.v1/t3","@type":"Dataset","description":"Observed 95% confidence-level upper limits on the cross section for Drell-Yan spin-1/2 monopole production as a function of mass for...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.89874.v1/t4","@type":"Dataset","description":"Observed 95% confidence-level upper limits on the cross section for Drell-Yan spin-1/2 HECO production as a function of mass for...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.89874.v1/t5","@type":"Dataset","description":"Selection efficiency as a function of transverse kinetic energy $E^\\text{kin}_\\text{T}=E_\\text{kin}\\sin\\theta$ and pseudorapidity $|\\eta|$ for $g=1g_\\textrm{D}$ monopoles of mass 200 GeV.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.89874.v1/t6","@type":"Dataset","description":"Selection efficiency as a function of transverse kinetic energy $E^\\text{kin}_\\text{T}=E_\\text{kin}\\sin\\theta$ and pseudorapidity $|\\eta|$ for $g=1g_\\textrm{D}$ monopoles of mass 500 GeV.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.89874.v1/t7","@type":"Dataset","description":"Selection efficiency as a function of transverse kinetic energy $E^\\text{kin}_\\text{T}=E_\\text{kin}\\sin\\theta$ and pseudorapidity $|\\eta|$ for $g=1g_\\textrm{D}$ monopoles of mass 1000 GeV.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.89874.v1/t8","@type":"Dataset","description":"Selection efficiency as a function of transverse kinetic energy $E^\\text{kin}_\\text{T}=E_\\text{kin}\\sin\\theta$ and pseudorapidity $|\\eta|$ for $g=1g_\\textrm{D}$ monopoles of mass 1500 GeV.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.89874.v1/t9","@type":"Dataset","description":"Selection efficiency as a function of transverse kinetic energy $E^\\text{kin}_\\text{T}=E_\\text{kin}\\sin\\theta$ and pseudorapidity $|\\eta|$ for $g=1g_\\textrm{D}$ monopoles of mass 2000 GeV.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.89874.v1/t10","@type":"Dataset","description":"Selection efficiency as a function of transverse kinetic energy $E^\\text{kin}_\\text{T}=E_\\text{kin}\\sin\\theta$ and pseudorapidity $|\\eta|$ for $g=1g_\\textrm{D}$ monopoles of mass 2500 GeV.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.89874.v1/t11","@type":"Dataset","description":"Selection efficiency as a function of transverse kinetic energy $E^\\text{kin}_\\text{T}=E_\\text{kin}\\sin\\theta$ and pseudorapidity $|\\eta|$ for $g=1g_\\textrm{D}$ monopoles of mass 3000 GeV.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.89874.v1/t12","@type":"Dataset","description":"Selection efficiency as a function of transverse kinetic energy $E^\\text{kin}_\\text{T}=E_\\text{kin}\\sin\\theta$ and pseudorapidity $|\\eta|$ for $g=1g_\\textrm{D}$ monopoles of mass 4000 GeV.","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.89874.v1/t13","@type":"Dataset","description":"Selection efficiency as a function of transverse kinetic energy $E^\\text{kin}_\\text{T}=E_\\text{kin}\\sin\\theta$ and pseudorapidity $|\\eta|$ for $g=2g_\\textrm{D}$ monopoles of mass 200 GeV.","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.89874.v1/t14","@type":"Dataset","description":"Selection efficiency as a function of transverse kinetic energy $E^\\text{kin}_\\text{T}=E_\\text{kin}\\sin\\theta$ and pseudorapidity $|\\eta|$ for $g=2g_\\textrm{D}$ monopoles of mass 500 GeV.","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.89874.v1/t15","@type":"Dataset","description":"Selection efficiency as a function of transverse kinetic energy $E^\\text{kin}_\\text{T}=E_\\text{kin}\\sin\\theta$ and pseudorapidity $|\\eta|$ for $g=2g_\\textrm{D}$ monopoles of mass 1000 GeV.","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.89874.v1/t16","@type":"Dataset","description":"Selection efficiency as a function of transverse kinetic energy $E^\\text{kin}_\\text{T}=E_\\text{kin}\\sin\\theta$ and pseudorapidity $|\\eta|$ for $g=2g_\\textrm{D}$ monopoles of mass 1500 GeV.","name":"Table 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19"},{"@id":"https://doi.org/10.17182/hepdata.89874.v1/t20","@type":"Dataset","description":"Selection efficiency as a function of transverse kinetic energy $E^\\text{kin}_\\text{T}=E_\\text{kin}\\sin\\theta$ and pseudorapidity $|\\eta|$ for $g=2g_\\textrm{D}$ monopoles of mass 4000 GeV.","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.89874.v1/t21","@type":"Dataset","description":"Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of...","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.89874.v1/t22","@type":"Dataset","description":"Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of...","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.89874.v1/t23","@type":"Dataset","description":"Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of...","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.89874.v1/t24","@type":"Dataset","description":"Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of...","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.89874.v1/t25","@type":"Dataset","description":"Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of...","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.89874.v1/t26","@type":"Dataset","description":"Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of...","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.89874.v1/t27","@type":"Dataset","description":"Total selection efficiency (i.e., the fraction of MC HECOs surviving the trigger and offline selection criteria) as a function of...","name":"Table 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