{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.140957.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2662587"}},{"@id":"https://doi.org/10.1007/JHEP10(2023)001","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2023","description":"A search for leptoquarks decaying into the $b\\tau$ final state  is performed using Run 2 proton-proton collision data from the Large Hadron Collider, corresponding to an integrated luminosity of 139 fb$^{-1}$ at $\\sqrt{s} = 13$ TeV recorded by the ATLAS detector. The benchmark models considered in this search are vector leptoquarks with electric charge of 2/3e and scalar leptoquarks with an electric charge of 4/3e.  No significant excess above the Standard Model prediction is observed, and 95% confidence level upper limits are set on the cross-section of leptoquarks decaying into $b\\tau$. For the vector leptoquark production two models are considered: the Yang-Mills and Minimal coupling models. In the Yang-Mills (Minimal coupling) scenario, vector leptoquarks with a mass below 1.58 (1.35) TeV are excluded for a gauge coupling of 1.0 and below 2.05 (1.99) TeV for a gauge coupling of 2.5. In the case of scalar leptoquarks, masses below 1.28 TeV (1.53 TeV) are excluded for a Yukawa coupling of 1.0 (2.5). Finally, an interpretation of the results with minimal model dependence is performed for each of the signal region categories, and limits on the  visible cross-section for beyond the Standard Model processes are provided.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t1","@type":"Dataset","description":"Observed (solid line) and expected (dashed line) 95% CL upper limits on the cross-section of single plus non-resonant plus pair...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t2","@type":"Dataset","description":"Observed (solid line) and expected (dashed line) 95% CL upper limits on the cross-section of single plus non-resonant plus pair...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t3","@type":"Dataset","description":"Observed (solid line) and expected (dashed line) 95% CL upper limits on the cross-section of single plus non-resonant plus pair...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t4","@type":"Dataset","description":"Observed (solid line) and expected (dashed line) 95% CL upper limits on the cross-section of single plus non-resonant plus pair...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t5","@type":"Dataset","description":"Observed (solid line) and expected (dashed line) 95% CL upper limits on the cross-section of single plus non-resonant plus pair...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t6","@type":"Dataset","description":"Observed (solid line) and expected (dashed line) 95% CL upper limits on the cross-section of single plus non-resonant plus pair...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t7","@type":"Dataset","description":"The two-dimensional 95% CL exclusion limits in the $\\lambda$-$m_{LQ}$ plane for singly plus non-resonant produced vector LQ (green lines) and...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t8","@type":"Dataset","description":"The two-dimensional 95% CL exclusion limits in the $\\lambda$-$m_{LQ}$ plane for singly plus non-resonant produced vector LQ (green lines) and...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t9","@type":"Dataset","description":"Observed (solid line) and expected (dashed line) 95% CL upper limits for $\\lambda$ = 1.0 on the cross-section of single...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t10","@type":"Dataset","description":"Observed (solid line) and expected (dashed line) 95% CL upper limits for $\\lambda$ = 1.7 on the cross-section of single...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t11","@type":"Dataset","description":"Observed (solid line) and expected (dashed line) 95% CL upper limits for $\\lambda$ = 2.5 on the cross-section of single...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t12","@type":"Dataset","description":"The two-dimensional 95% CL exclusion limits in the $\\lambda$-$m_{LQ}$ plane for singly plus non-resonant produced $\\widetilde{S_{1}}$ (green lines) and for...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t13","@type":"Dataset","description":"Observed (solid line) and expected (dashed line) 95% upper limits on the visible cross-section, $\\sigma_{\\mathrm{vis}}$, obtained from model-independent search by...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t14","@type":"Dataset","description":"Observed (solid line) and expected (dashed line) 95% CL upper limits on the cross-section of singly plus non-resonant produced vector...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t15","@type":"Dataset","description":"Observed (solid line) and expected (dashed line) 95% CL upper limits on the cross-section of singly plus non-resonant produced vector...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t16","@type":"Dataset","description":"Observed (solid line) and expected (dashed line) 95% CL upper limits on the cross-section of singly plus non-resonant produced vector...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t17","@type":"Dataset","description":"Observed (solid line) and expected (dashed line) 95% CL upper limits on the cross-section of singly plus non-resonant produced vector...","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t18","@type":"Dataset","description":"Observed (solid line) and expected (dashed line) 95% CL upper limits on the cross-section of singly plus non-resonant produced vector...","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t19","@type":"Dataset","description":"Observed (solid line) and expected (dashed line) 95% CL upper limits on the cross-section of singly plus non-resonant produced vector...","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t20","@type":"Dataset","description":"Observed (solid line) and expected (dashed line) 95% CL upper limits for $\\lambda$ = 1.0 on the cross-section of singly...","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t21","@type":"Dataset","description":"Observed (solid line) and expected (dashed line) 95% CL upper limits for $\\lambda$ = 1.7 on the cross-section of singly...","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t22","@type":"Dataset","description":"Observed (solid line) and expected (dashed line) 95% CL upper limits for $\\lambda$ = 2.5 on the cross-section of singly...","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t23","@type":"Dataset","description":"The signal acceptance times efficiency for single plus non-resonant produced LQ in the $\\widetilde{S_{1}}$ model from the combination of the...","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t24","@type":"Dataset","description":"The signal acceptance times efficiency for single plus non-resonant produced LQ in the $\\widetilde{S_{1}}$ model from the combination of the...","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t25","@type":"Dataset","description":"The signal acceptance times efficiency for single plus non-resonant produced LQ in the $\\widetilde{S_{1}}$ model from the combination of the...","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t26","@type":"Dataset","description":"The signal acceptance times efficiency for single plus non-resonant produced LQ in the $U_1^{MIN}$ model from the combination of the...","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t27","@type":"Dataset","description":"The signal acceptance times efficiency for single plus non-resonant produced LQ in the $U_1^{MIN}$ model from the combination of the...","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t28","@type":"Dataset","description":"The signal acceptance times efficiency for single plus non-resonant produced LQ in the $U_1^{MIN}$ model from the combination of the...","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t29","@type":"Dataset","description":"The signal acceptance times efficiency for single plus non-resonant produced LQ in the $U_1^{YM}$ model from the combination of the...","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t30","@type":"Dataset","description":"The signal acceptance times efficiency for single plus non-resonant produced LQ in the $U_1^{YM}$ model from the combination of the...","name":"Table 30"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t31","@type":"Dataset","description":"The signal acceptance times efficiency for single plus non-resonant produced LQ in the $U_1^{YM}$ model from the combination of the...","name":"Table 31"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t32","@type":"Dataset","description":"Observed (solid line) and expected (dashed line) 95% CL upper limits on the cross-section of singly produced vector LQ signals...","name":"Table 32"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t33","@type":"Dataset","description":"Observed (solid line) and expected (dashed line) 95% CL upper limits on the cross-section of singly produced vector LQ signals...","name":"Table 33"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t34","@type":"Dataset","description":"Observed (solid line) and expected (dashed line) 95% CL upper limits on the cross-section of singly produced vector LQ signals...","name":"Table 34"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t35","@type":"Dataset","description":"Observed (solid line) and expected (dashed line) 95% CL upper limits on the cross-section of singly produced vector LQ signals...","name":"Table 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47"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t48","@type":"Dataset","description":"Observed (solid line) and expected (dashed line) 95% CL upper limits for $\\lambda$ = 2.5 on the cross-section of singly-produced...","name":"Table 48"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t49","@type":"Dataset","description":"Observed (solid line) and expected (dashed line) 95% CL upper limits for $\\lambda$ = 1.0 on the cross-section of single...","name":"Table 49"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t50","@type":"Dataset","description":"Observed (solid line) and expected (dashed line) 95% CL upper limits for $\\lambda$ = 1.7 on the cross-section of single...","name":"Table 50"},{"@id":"https://doi.org/10.17182/hepdata.140957.v1/t51","@type":"Dataset","description":"Observed (solid line) and expected (dashed line) 95% CL upper limits for $\\lambda$ = 2.5 on the cross-section of single...","name":"Table 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