{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.98627.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1844425"}},{"@id":"https://doi.org/10.1007/JHEP04(2021)165","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2021","description":"The results of a search for direct pair production of top squarks and for dark matter in events with two opposite-charge leptons (electrons or muons), jets and missing transverse momentum are reported, using 139~\\mbox{fb\\(^{-1}\\)} of integrated luminosity from proton--proton collisions at $\\sqrt{s}=13$ TeV, collected by the ATLAS detector at the Large Hadron Collider during Run~2 (2015--2018). This search considers the pair production of top squarks and is sensitive across a wide range of mass differences between the top squark and the lightest neutralino. Additionally, spin-0 mediator dark-matter models are considered, in which the mediator is produced in association with a pair of top quarks. The mediator subsequently decays to a pair of dark-matter particles. No significant excess of events is observed above the Standard Model background, and limits are set at $95\\%$\\ confidence level. The results exclude  top squark masses up to about $1$ TeV, and masses of the lightest neutralino up to about $500$ GeV. Limits on dark-matter production are set for scalar (pseudoscalar) mediator  masses up to about $250~(300)$ GeV.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.98627.v1/t1","@type":"Dataset","description":"Two-body selection. 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Distributions of $M_{\\Delta}^R$ in (a,b) $SR_{W}^{3-body}$ and (c,d) $SR_{T}^{3-body}$ for (left) same-flavour and (right) different-flavour events satisfying the...","name":"Figure 12b"},{"@id":"https://doi.org/10.17182/hepdata.98627.v1/t5","@type":"Dataset","description":"Three-body selection. Distributions of $M_{\\Delta}^R$ in (a,b) $SR_{W}^{3-body}$ and (c,d) $SR_{T}^{3-body}$ for (left) same-flavour and (right) different-flavour events satisfying the...","name":"Figure 12c"},{"@id":"https://doi.org/10.17182/hepdata.98627.v1/t6","@type":"Dataset","description":"Three-body selection. Distributions of $M_{\\Delta}^R$ in (a,b) $SR_{W}^{3-body}$ and (c,d) $SR_{T}^{3-body}$ for (left) same-flavour and (right) different-flavour events satisfying the...","name":"Figure 12d"},{"@id":"https://doi.org/10.17182/hepdata.98627.v1/t7","@type":"Dataset","description":"Four-body selection. (a) distributions of $E_{T}^{miss}$ in $SR^{4-body}_{Small\\,\\Delta m}$ and (b) distribution of $R_{2\\ell 4j}$ in $SR^{4-body}_{Large\\,\\Delta m}$ for events...","name":"Figure 13a"},{"@id":"https://doi.org/10.17182/hepdata.98627.v1/t8","@type":"Dataset","description":"Four-body selection. (a) distributions of $E_{T}^{miss}$ in $SR^{4-body}_{Small\\,\\Delta m}$ and (b) distribution of $R_{2\\ell 4j}$ in $SR^{4-body}_{Large\\,\\Delta m}$ for events...","name":"Figure 13b"},{"@id":"https://doi.org/10.17182/hepdata.98627.v1/t9","@type":"Dataset","description":"Exclusion limit contour (95% CL) for a simplified model assuming $\\tilde{t}_1$ pair production, decaying via $\\tilde{t}_1 \\rightarrow t^{(*)}\\tilde{\\chi}_1^0$ with 100%...","name":"Figure 14a - Expected limits"},{"@id":"https://doi.org/10.17182/hepdata.98627.v1/t10","@type":"Dataset","description":"Exclusion limit contour (95% CL) for a simplified model assuming $\\tilde{t}_1$ pair production, decaying via $\\tilde{t}_1 \\rightarrow t^{(*)}\\tilde{\\chi}_1^0$ with 100%...","name":"Figure 14a - Expected limits Up 1 sigma"},{"@id":"https://doi.org/10.17182/hepdata.98627.v1/t11","@type":"Dataset","description":"Exclusion limit contour (95% CL) for a simplified model assuming $\\tilde{t}_1$ pair production, decaying via $\\tilde{t}_1 \\rightarrow t^{(*)}\\tilde{\\chi}_1^0$ with 100%...","name":"Figure 14a - 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Observed limits Down 1 sigma"},{"@id":"https://doi.org/10.17182/hepdata.98627.v1/t20","@type":"Dataset","description":"Exclusion limit contour (95% CL) for a simplified model assuming $\\tilde{t}_1$ pair production, decaying via $\\tilde{t}_1 \\rightarrow t^{(*)}\\tilde{\\chi}_1^0$ with 100\\%...","name":"Figure 14b - Observed limits Up 1 sigma"},{"@id":"https://doi.org/10.17182/hepdata.98627.v1/t21","@type":"Dataset","description":"Exclusion limits for (a) $t\\bar{t} + \\phi $ scalar and (b) $t\\bar{t} + a $ pseudoscalar models as a function...","name":"Figure 15a - Expected limits"},{"@id":"https://doi.org/10.17182/hepdata.98627.v1/t22","@type":"Dataset","description":"Exclusion limits for (a) $t\\bar{t} + \\phi $ scalar and (b) $t\\bar{t} + a $ pseudoscalar models as a function...","name":"Figure 15a - Observed limits"},{"@id":"https://doi.org/10.17182/hepdata.98627.v1/t23","@type":"Dataset","description":"Exclusion limits for (a) $t\\bar{t} + \\phi $ scalar and (b) $t\\bar{t} + a $ pseudoscalar models as a function...","name":"Figure 15b - 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Background fit results for $\\mathrm{CR}^{\\mathrm{2-body}}_{t\\bar{t}}$, $\\mathrm{CR}^{\\mathrm{2-body}}_{t\\bar{t}Z}$, $\\mathrm{VR}^{\\mathrm{2-body}}_{t\\bar{t}, DF}$, $\\mathrm{VR}^{\\mathrm{2-body}}_{t\\bar{t}, SF}$ and $\\mathrm{VR}^{\\mathrm{2-body}}_{t\\bar{t} Z}$. ''Others'' includes contributions from $VVV$,...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.98627.v1/t26","@type":"Dataset","description":"Three-body selection. Background fit results for $\\mathrm{CR}^{\\mathrm{3-body}}_{t\\bar{t}}$, $\\mathrm{CR}^{\\mathrm{3-body}}_{VV}$, $\\mathrm{CR}^{\\mathrm{2-body}}_{t\\bar{t}Z}$, $\\mathrm{VR}^{\\mathrm{3-body}}_{VV}$, $\\mathrm{VR(1)}^{\\mathrm{3-body}}_{t\\bar{t}}$ and $\\mathrm{VR(2)}^{\\mathrm{3-body}}_{t\\bar{t}}$. ''Others'' includes contributions from $VVV$, $t\\bar{t} t$,...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.98627.v1/t27","@type":"Dataset","description":"Four-body selection. Background fit results for $\\mathrm{CR}^{\\mathrm{4-body}}_{t\\bar{t}}$,$\\mathrm{CR}^{\\mathrm{4-body}}_{VV}$, $\\mathrm{VR}^{\\mathrm{4-body}}_{t\\bar{t}}$, $VR^{4-body}_{VV}$ and $\\mathrm{VR}^{\\mathrm{4-body}}_{VV,lll}$. The ''Others'' category contains the contributions from $VVV$, $t\\bar{t}...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.98627.v1/t28","@type":"Dataset","description":"Two-body selection. Background fit results for the different-flavour leptons binned SRs. The ''Others'' category contains the contributions from $VVV$, $t\\bar{t}...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.98627.v1/t29","@type":"Dataset","description":"Two-body selection. Background fit results for the same-flavour leptons binned SRs. The ''Others'' category contains the contributions from $VVV$, $t\\bar{t}...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.98627.v1/t30","@type":"Dataset","description":"Three-body selection. 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Fig. 10(c): Efficiency SUSY 2-body SRDF2"},{"@id":"https://doi.org/10.17182/hepdata.98627.v1/t53","@type":"Dataset","description":"Two-body selection efficiency (a) SR-DF$^{2-body}_{[110,120)}$, (b) SR-DF1$^{2-body}_{[120,140)}$, (c) SR-DF2$^{2-body}_{[140,160)}$, (d) SR-DF3$^{2-body}_{[160,180)}$, (e) SR-DF4$^{2-body}_{[180,220)}$, (f) SR-DF5$^{2-body}_{[220,\\infty)}$ for a simplified model assuming...","name":"Aux. Fig. 10(d): Efficiency SUSY 2-body SRDF3"},{"@id":"https://doi.org/10.17182/hepdata.98627.v1/t54","@type":"Dataset","description":"Two-body selection efficiency (a) SR-DF$^{2-body}_{[110,120)}$, (b) SR-DF1$^{2-body}_{[120,140)}$, (c) SR-DF2$^{2-body}_{[140,160)}$, (d) SR-DF3$^{2-body}_{[160,180)}$, (e) SR-DF4$^{2-body}_{[180,220)}$, (f) SR-DF5$^{2-body}_{[220,\\infty)}$ for a simplified model assuming...","name":"Aux. 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Fig. 11(c): Efficiency SUSY 2-body SRSF2"},{"@id":"https://doi.org/10.17182/hepdata.98627.v1/t59","@type":"Dataset","description":"Two-body selection efficiency (a) SR-SF$^{2-body}_{[110,120)}$, (b) SR-SF1$^{2-body}_{[120,140)}$, (c) SR-SF2$^{2-body}_{[140,160)}$, (d) SR-SF3$^{2-body}_{[160,180)}$, (e) SR-SF4$^{2-body}_{[180,220)}$, (f) SR-SF5$^{2-body}_{[220,\\infty)}$ for a simplified model assuming...","name":"Aux. Fig. 11(d): Efficiency SUSY 2-body SRSF3"},{"@id":"https://doi.org/10.17182/hepdata.98627.v1/t60","@type":"Dataset","description":"Two-body selection efficiency (a) SR-SF$^{2-body}_{[110,120)}$, (b) SR-SF1$^{2-body}_{[120,140)}$, (c) SR-SF2$^{2-body}_{[140,160)}$, (d) SR-SF3$^{2-body}_{[160,180)}$, (e) SR-SF4$^{2-body}_{[180,220)}$, (f) SR-SF5$^{2-body}_{[220,\\infty)}$ for a simplified model assuming...","name":"Aux. 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