{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.141286.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2686746"}},{"@id":"https://doi.org/10.1007/JHEP11(2023)112","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2023","description":"CERN-LHC. We present a search for magnetic monopoles and high-electric-charge objects using LHC Run 2 $\\sqrt{s}$ = 13 TeV proton\u2013proton collisions recorded by the ATLAS detector. A total integrated luminosity of 138 fb$^{\u22121}$ was collected by a specialized trigger and analyzed.No highly ionizing particle candidate was observed. Considering the Drell-Yan and photon-fusion pair production mechanisms as benchmark models, lowest to-date cross-section upper limits are presented for spin-0 and spin-$\\frac{1}{2}$ magnetic monopoles of charge 1$g_{D}$ and 2$g_{D}$ and high-electric-charge objects of charge $20\\le|z|\\le100$, for masses between 200 and 4000 GeV.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t1","@type":"Dataset","description":"Observed 95% CL upper limits on the cross section for all masses and charges of Drell-Yan spin-0 monopoles production as...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t2","@type":"Dataset","description":"Observed 95% CL upper limits on the cross section for all masses and charges of Drell-Yan spin-1/2 monopoles production as...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t3","@type":"Dataset","description":"Observed 95% CL upper limits on the cross section for all masses and charges of photon-fusion pair-produced spin-0 monopoles as...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t4","@type":"Dataset","description":"Observed 95% CL upper limits on the cross section for all masses and charges of photon-fusion pair-produced spin-1/2 monopoles as...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t5","@type":"Dataset","description":"Observed 95% CL upper limits on the cross section for all masses and charges of Drell-Yan spin-0 HECOs production as...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t6","@type":"Dataset","description":"Observed 95% CL upper limits on the cross section for all masses and charges of Drell-Yan spin-1/2 HECOs production as...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t7","@type":"Dataset","description":"Observed 95% CL upper limits on the cross section for all masses and charges of photon-fusion pair-produced spin-0 HECOs as...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t8","@type":"Dataset","description":"Observed 95% CL upper limits on the cross section for all masses and charges of photon-fusion pair-produced spin-1/2 HECOs as...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.141286.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 200 GeV.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.141286.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 500 GeV.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.141286.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 1000 GeV.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.141286.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 1500 GeV.","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.141286.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 $g=1g_\\textrm{D}$ monopoles of mass 2000 GeV.","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.141286.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 $g=1g_\\textrm{D}$ monopoles of mass 2500 GeV.","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.141286.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 $g=1g_\\textrm{D}$ monopoles of mass 3000 GeV.","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.141286.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 $g=1g_\\textrm{D}$ monopoles of mass 4000 GeV.","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t17","@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 17"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t18","@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 18"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t19","@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 19"},{"@id":"https://doi.org/10.17182/hepdata.141286.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 1500 GeV.","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t21","@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 2000 GeV.","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t22","@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 2500 GeV.","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t23","@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 3000 GeV.","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t24","@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 24"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t25","@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 HECOs of charge $|z|=20$ of mass...","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t26","@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 HECOs of charge $|z|=20$ of mass...","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t27","@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 HECOs of charge $|z|=20$ of mass...","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t28","@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 HECOs of charge $|z|=20$ of mass...","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t29","@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 HECOs of charge $|z|=20$ of mass...","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t30","@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 HECOs of charge $|z|=20$ of mass...","name":"Table 30"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t31","@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 HECOs of charge $|z|=20$ of mass...","name":"Table 31"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t32","@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 HECOs of charge $|z|=20$ of mass...","name":"Table 32"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t33","@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 HECOs of charge $|z|=40$ of mass...","name":"Table 33"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t34","@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 HECOs of charge $|z|=40$ of mass...","name":"Table 34"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t35","@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 HECOs of charge $|z|=40$ of mass...","name":"Table 35"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t36","@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 HECOs of charge $|z|=40$ of mass...","name":"Table 36"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t37","@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 HECOs of charge $|z|=40$ of mass...","name":"Table 37"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t38","@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 HECOs of charge $|z|=40$ of mass...","name":"Table 38"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t39","@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 HECOs of charge $|z|=40$ of mass...","name":"Table 39"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t40","@type":"Dataset","description":"Selection efficiency as a function of transverse kinetic energy $E^\\text{kin}_\\text{T}=E_\\text{kin}\\sin\\theta$ and pseudorapidity 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a function of transverse kinetic energy $E^\\text{kin}_\\text{T}=E_\\text{kin}\\sin\\theta$ and pseudorapidity $|\\eta|$ for HECOs of charge $|z|=60$ of mass...","name":"Table 47"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t48","@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 HECOs of charge $|z|=60$ of mass...","name":"Table 48"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t49","@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 HECOs of charge $|z|=80$ of mass...","name":"Table 49"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t50","@type":"Dataset","description":"Selection efficiency as a function of transverse kinetic energy $E^\\text{kin}_\\text{T}=E_\\text{kin}\\sin\\theta$ and pseudorapidity 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a function of transverse kinetic energy $E^\\text{kin}_\\text{T}=E_\\text{kin}\\sin\\theta$ and pseudorapidity $|\\eta|$ for HECOs of charge $|z|=100$ of mass...","name":"Table 57"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t58","@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 HECOs of charge $|z|=100$ of mass...","name":"Table 58"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t59","@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 HECOs of charge $|z|=100$ of mass...","name":"Table 59"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t60","@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 HECOs of charge $|z|=100$ of mass...","name":"Table 60"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t61","@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 HECOs of charge $|z|=100$ of mass...","name":"Table 61"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t62","@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 HECOs of charge $|z|=100$ of mass...","name":"Table 62"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t63","@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 HECOs of charge $|z|=100$ of mass...","name":"Table 63"},{"@id":"https://doi.org/10.17182/hepdata.141286.v1/t64","@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 HECOs of charge $|z|=100$ of mass...","name":"Table 64"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2686746?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/141286"}],"inLanguage":"en","name":"Search for magnetic monopoles and stable particles with high electric charges in $\\sqrt{s}=$13 TeV $pp$ collisions with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2686746?version=1","version":1}