cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.140436.v1/t2
title: "Figure 3a" of "Bose-Einstein correlations of charged pion pairs in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: The $k_T$ dependence of the Bertsch-Pratt radius parameters and $\lambda$ for charged pions for 0-30% centrality. Filled triangles show the results from fits to a core-halo structure by Eq. 2, with statistical error bars and systematic error bands. Open circles and squares show the results from the full (Eq. 1) and 50% partial (Eq. 3) Coulomb corrections with statistical error bars, respectively. Results at 130 GeV by PHENIX are given by filled circles.
description: Bose-Einstein correlations of identically ch√arged pion pairs were measured by the PHENIX experiment at mid-rapidity in Au + Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The Bertsch-Pratt radius parameters were determined as a function of the transverse momentum of the pair and as a function of the centrality of the collision. Using the full Coulomb correction, the ratio $R_{out}$/$R_{side}$ is smaller than unity for $⟨k_T⟩$ from 0.25 to 1.2 GeV/$c$ and for all measured centralities. However, using recently developed partial Coulomb correction methods, we find that $R_{out}$/$R_{side}$ is 0.8-1.1 for the measured $⟨k_T⟩$ range, and approximately constant at unity with the number of participants.
DOI: 10.17182/hepdata.140436.v1/t3
title: "Figure 3b" of "Bose-Einstein correlations of charged pion pairs in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: The $k_T$ dependence of the Bertsch-Pratt radius parameters and $\lambda$ for charged pions for 0-30% centrality. Filled triangles show the results from fits to a core-halo structure by Eq. 2, with statistical error bars and systematic error bands. Open circles and squares show the results from the full (Eq. 1) and 50% partial (Eq. 3) Coulomb corrections with statistical error bars, respectively. Results at 130 GeV by PHENIX are given by filled circles.
description: Bose-Einstein correlations of identically ch√arged pion pairs were measured by the PHENIX experiment at mid-rapidity in Au + Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The Bertsch-Pratt radius parameters were determined as a function of the transverse momentum of the pair and as a function of the centrality of the collision. Using the full Coulomb correction, the ratio $R_{out}$/$R_{side}$ is smaller than unity for $⟨k_T⟩$ from 0.25 to 1.2 GeV/$c$ and for all measured centralities. However, using recently developed partial Coulomb correction methods, we find that $R_{out}$/$R_{side}$ is 0.8-1.1 for the measured $⟨k_T⟩$ range, and approximately constant at unity with the number of participants.
DOI: 10.17182/hepdata.140436.v1/t4
title: "Figure 4a" of "Bose-Einstein correlations of charged pion pairs in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Bertsch-Pratt radius parameters versus the cube root of the number of participants ($N^{1/3}_{part}$) for $\pi^+\pi^+$ (blue squares) and $\pi^-\pi^-$ (red triangle) for the fits to a core-halo structure by Eq. (2) with statistical error bars and systematic error bands, in the 0.2 GeV/$c$ &lt; $k_T$ &lt; 2.0 GeV/$c$ range, with $$ ~ 0.45 GeV/$c$. The solid line shows to $p_0$+$p_1$*$N^{1/3}_{part}$ for both signs.
description: Bose-Einstein correlations of identically ch√arged pion pairs were measured by the PHENIX experiment at mid-rapidity in Au + Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The Bertsch-Pratt radius parameters were determined as a function of the transverse momentum of the pair and as a function of the centrality of the collision. Using the full Coulomb correction, the ratio $R_{out}$/$R_{side}$ is smaller than unity for $⟨k_T⟩$ from 0.25 to 1.2 GeV/$c$ and for all measured centralities. However, using recently developed partial Coulomb correction methods, we find that $R_{out}$/$R_{side}$ is 0.8-1.1 for the measured $⟨k_T⟩$ range, and approximately constant at unity with the number of participants.
DOI: 10.17182/hepdata.140436.v1/t5
title: "Figure 4b" of "Bose-Einstein correlations of charged pion pairs in Au + Au collisions at s(NN)**(1/2) = 200-GeV."

description: Bertsch-Pratt radius parameters versus the cube root of the number of participants ($N^{1/3}_{part}$) for $\pi^+\pi^+$ (blue squares) and $\pi^-\pi^-$ (red triangle) for the fits to a core-halo structure by Eq. (2) with statistical error bars and systematic error bands, in the 0.2 GeV/$c$ &lt; $k_T$ &lt; 2.0 GeV/$c$ range, with $$ ~ 0.45 GeV/$c$. The solid line shows to $p_0$+$p_1$*$N^{1/3}_{part}$ for both signs.
description: Bose-Einstein correlations of identically ch√arged pion pairs were measured by the PHENIX experiment at mid-rapidity in Au + Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The Bertsch-Pratt radius parameters were determined as a function of the transverse momentum of the pair and as a function of the centrality of the collision. Using the full Coulomb correction, the ratio $R_{out}$/$R_{side}$ is smaller than unity for $⟨k_T⟩$ from 0.25 to 1.2 GeV/$c$ and for all measured centralities. However, using recently developed partial Coulomb correction methods, we find that $R_{out}$/$R_{side}$ is 0.8-1.1 for the measured $⟨k_T⟩$ range, and approximately constant at unity with the number of participants.
DOI: 10.17182/hepdata.140485.v1/t1
title: "Table 1" of "First measurement of $\Lambda_\mathrm{c}^{+}$ production down to $p_\mathrm{T} = 0$ in pp and p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV"

description: The $p_\mathrm{T}$-differential prompt $\Lambda_\mathrm{c}^{+}$ production cross sections per unit rapidity in pp collisions for $|y| &lt; 0.5$, at $\sqrt{s} = 5.02$ TeV. Data for $1
description: The production of prompt $\Lambda_\mathrm{c}^+$ baryons has been measured at midrapidity in the transverse momentum interval $0
DOI: 10.17182/hepdata.140485.v1/t2
title: "Table 2" of "First measurement of $\Lambda_\mathrm{c}^{+}$ production down to $p_\mathrm{T} = 0$ in pp and p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV"

description: The $p_\mathrm{T}$-differential prompt $\Lambda_\mathrm{c}^{+}$ production cross sections per unit rapidity in p-Pb collisions for $-0.96
description: The production of prompt $\Lambda_\mathrm{c}^+$ baryons has been measured at midrapidity in the transverse momentum interval $0
DOI: 10.17182/hepdata.140485.v1/t3
title: "Table 3" of "First measurement of $\Lambda_\mathrm{c}^{+}$ production down to $p_\mathrm{T} = 0$ in pp and p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV"

description: The $p_\mathrm{T}$-integrated production cross sections per unit rapidity for prompt $\Lambda_\mathrm{c}^{+}$ baryons in pp and p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV.
description: The production of prompt $\Lambda_\mathrm{c}^+$ baryons has been measured at midrapidity in the transverse momentum interval $0
DOI: 10.17182/hepdata.140485.v1/t4
title: "Table 4" of "First measurement of $\Lambda_\mathrm{c}^{+}$ production down to $p_\mathrm{T} = 0$ in pp and p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV"

description: The nuclear modification factor $R_\mathrm{pPb}$ for prompt $\Lambda_\mathrm{c}^{+}$ production in p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV. Data for $1
description: The production of prompt $\Lambda_\mathrm{c}^+$ baryons has been measured at midrapidity in the transverse momentum interval $0
DOI: 10.17182/hepdata.140485.v1/t5
title: "Table 5" of "First measurement of $\Lambda_\mathrm{c}^{+}$ production down to $p_\mathrm{T} = 0$ in pp and p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV"

description: The $p_\mathrm{T}$-integrated nuclear modification factors $R_\mathrm{pPb}$ and $R_\mathrm{AA}$ for prompt $\Lambda_\mathrm{c}^{+}$ production in p-Pb and Pb-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV.
description: The production of prompt $\Lambda_\mathrm{c}^+$ baryons has been measured at midrapidity in the transverse momentum interval $0
DOI: 10.17182/hepdata.140485.v1/t6
title: "Table 6" of "First measurement of $\Lambda_\mathrm{c}^{+}$ production down to $p_\mathrm{T} = 0$ in pp and p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV"

description: Mean transverse momentum values for prompt $\Lambda_\mathrm{c}^{+}$ baryons at midrapidity in pp and p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV.
description: The production of prompt $\Lambda_\mathrm{c}^+$ baryons has been measured at midrapidity in the transverse momentum interval $0
DOI: 10.17182/hepdata.140485.v1/t7
title: "Table 7" of "First measurement of $\Lambda_\mathrm{c}^{+}$ production down to $p_\mathrm{T} = 0$ in pp and p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV"

description: The prompt $\Lambda_{\rm {c}}^{+}$/${\rm D}^{0}$ yield ratio measured in pp collisions at $\sqrt{s} = 5.02$ TeV as a function of $p_\mathrm{T}$. Data for $1
description: The production of prompt $\Lambda_\mathrm{c}^+$ baryons has been measured at midrapidity in the transverse momentum interval $0
DOI: 10.17182/hepdata.140485.v1/t8
title: "Table 8" of "First measurement of $\Lambda_\mathrm{c}^{+}$ production down to $p_\mathrm{T} = 0$ in pp and p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV"

description: The prompt $\Lambda_{\rm {c}}^{+}$/${\rm D}^{0}$ yield ratio measured in p-Pb collisions at $\sqrt{s_{\rm {NN}}} = 5.02$ TeV as a function of $p_\mathrm{T}$. Data for $1
description: The production of prompt $\Lambda_\mathrm{c}^+$ baryons has been measured at midrapidity in the transverse momentum interval $0
DOI: 10.17182/hepdata.140485.v1/t9
title: "Table 9" of "First measurement of $\Lambda_\mathrm{c}^{+}$ production down to $p_\mathrm{T} = 0$ in pp and p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV"

description: The integrated prompt $\Lambda_\mathrm{c}^{+}/\mathrm{D}^0$ baryon-to-meson yield ratios in pp and p-Pb collisions at $\sqrt{s_{\rm {NN}}} = 5.02$ TeV.
description: The production of prompt $\Lambda_\mathrm{c}^+$ baryons has been measured at midrapidity in the transverse momentum interval $0
DOI: 10.17182/hepdata.140524.v1/t1
title: "Cross section" of "$J/\psi$ and $\psi(2S)$ production at forward rapidity in $p$+$p$ collisions at $\sqrt{s}=510$ GeV"

description: The total cross section times the branching ratio.
description: The PHENIX experiment at the Relativistic Heavy Ion Collider has measured the differential cross section, mean transverse momentum, mean transverse momentum squared of inclusive $J/\psi$ and cross-section ratio of $\psi(2S)$ to $J/\psi$ at forward rapidity in $p$+$p$ collisions at $\sqrt{s}$ = 510 GeV via the dimuon decay channel. Comparison is made to inclusive $J/\psi$ cross sections measured at $\sqrt{s}$ = 200 GeV and 2.76-13 TeV. The result is also compared to leading-order nonrelativistic QCD calculations coupled to a color-glass-condensate description of the low-$x$ gluons in the proton at low transverse momentum ($p_T$) and to next-to-leading order nonrelativistic QCD calculations for the rest of the $p_T$ range. These calculations overestimate the data at low $p_T$. While consistent with the data within uncertainties above ≈ 3 GeV/$c$, the calculations are systematically below the data. The total cross section times the branching ratio is BR $d{\sigma^{J/\psi}_{pp}}/dy$(1.2 &lt; $|y|$ &lt; 2.2, 0 &lt; $p_T$ &lt; 10 GeV/$c$) = 54.3 $\pm$ 0.5 (stat) $\pm$ 5.5 (syst) nb.
DOI: 10.17182/hepdata.140524.v1/t2
title: "Figure 5" of "$J/\psi$ and $\psi(2S)$ production at forward rapidity in $p$+$p$ collisions at $\sqrt{s}=510$ GeV"

description: The inclusive $J/\psi$ differential cross section as a function of $p_T$ at 1.2 &lt; $|y|$ &lt; 2.2 at 510 GeV.
description: The PHENIX experiment at the Relativistic Heavy Ion Collider has measured the differential cross section, mean transverse momentum, mean transverse momentum squared of inclusive $J/\psi$ and cross-section ratio of $\psi(2S)$ to $J/\psi$ at forward rapidity in $p$+$p$ collisions at $\sqrt{s}$ = 510 GeV via the dimuon decay channel. Comparison is made to inclusive $J/\psi$ cross sections measured at $\sqrt{s}$ = 200 GeV and 2.76-13 TeV. The result is also compared to leading-order nonrelativistic QCD calculations coupled to a color-glass-condensate description of the low-$x$ gluons in the proton at low transverse momentum ($p_T$) and to next-to-leading order nonrelativistic QCD calculations for the rest of the $p_T$ range. These calculations overestimate the data at low $p_T$. While consistent with the data within uncertainties above ≈ 3 GeV/$c$, the calculations are systematically below the data. The total cross section times the branching ratio is BR $d{\sigma^{J/\psi}_{pp}}/dy$(1.2 &lt; $|y|$ &lt; 2.2, 0 &lt; $p_T$ &lt; 10 GeV/$c$) = 54.3 $\pm$ 0.5 (stat) $\pm$ 5.5 (syst) nb.
DOI: 10.17182/hepdata.140524.v1/t3
title: "Figure 6" of "$J/\psi$ and $\psi(2S)$ production at forward rapidity in $p$+$p$ collisions at $\sqrt{s}=510$ GeV"

description: The inclusive $J/\psi$ differential cross section integrated over 0 &lt; $p_T$ &lt; 10 GeV/$c$ as a function of rapidity at 510 GeV.
description: The PHENIX experiment at the Relativistic Heavy Ion Collider has measured the differential cross section, mean transverse momentum, mean transverse momentum squared of inclusive $J/\psi$ and cross-section ratio of $\psi(2S)$ to $J/\psi$ at forward rapidity in $p$+$p$ collisions at $\sqrt{s}$ = 510 GeV via the dimuon decay channel. Comparison is made to inclusive $J/\psi$ cross sections measured at $\sqrt{s}$ = 200 GeV and 2.76-13 TeV. The result is also compared to leading-order nonrelativistic QCD calculations coupled to a color-glass-condensate description of the low-$x$ gluons in the proton at low transverse momentum ($p_T$) and to next-to-leading order nonrelativistic QCD calculations for the rest of the $p_T$ range. These calculations overestimate the data at low $p_T$. While consistent with the data within uncertainties above ≈ 3 GeV/$c$, the calculations are systematically below the data. The total cross section times the branching ratio is BR $d{\sigma^{J/\psi}_{pp}}/dy$(1.2 &lt; $|y|$ &lt; 2.2, 0 &lt; $p_T$ &lt; 10 GeV/$c$) = 54.3 $\pm$ 0.5 (stat) $\pm$ 5.5 (syst) nb.
DOI: 10.17182/hepdata.140528.v1/t1
title: "Figure 2a" of "Search for new Higgs bosons via same-sign top quark pair production in association with a jet in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Pre-fit distributon for leading jet's CvsL variable.
description: No data abstract available.
DOI: 10.17182/hepdata.140528.v1/t2
title: "Figure 2b" of "Search for new Higgs bosons via same-sign top quark pair production in association with a jet in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Pre-fit distributon for leading jet's CvsB variable.
description: No data abstract available.
DOI: 10.17182/hepdata.140528.v1/t3
title: "Figure 3a" of "Search for new Higgs bosons via same-sign top quark pair production in association with a jet in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Post-fit distributon of BDT discriminants for $\rho_{tu}=1.0$ with $m_A$ = 350 GeV interfered with H.($m_A - m_H$ = 50 GeV)
description: No data abstract available.
DOI: 10.17182/hepdata.140528.v1/t4
title: "Figure 3b" of "Search for new Higgs bosons via same-sign top quark pair production in association with a jet in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Post-fit distributon of BDT discriminants for $\rho_{tc}=1.0$ with $m_A$ = 350 GeV interfered with H.($m_A - m_H$ = 50 GeV)
description: No data abstract available.
DOI: 10.17182/hepdata.140528.v1/t5
title: "Figure 4a" of "Search for new Higgs bosons via same-sign top quark pair production in association with a jet in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed and expected 95% CL upper limit on the signal strength as a function of $m_A$ for the g2HDM signal model using different coupling assumptions: $\rho_{tu}$ = 0.1, 0.4, 1.0.
description: No data abstract available.
DOI: 10.17182/hepdata.140528.v1/t10
title: "Figure 6a(expected exclusion)" of "Search for new Higgs bosons via same-sign top quark pair production in association with a jet in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected exclusion as a function of $m_A$ and $\rho_{tu}$ for the g2HDM signal model
description: No data abstract available.
DOI: 10.17182/hepdata.140528.v1/t11
title: "Figure 6a(observed exclusion)" of "Search for new Higgs bosons via same-sign top quark pair production in association with a jet in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed exclusion as a function of $m_A$ and $\rho_{tu}$ for the g2HDM signal model
description: No data abstract available.
DOI: 10.17182/hepdata.140528.v1/t6
title: "Figure 4b" of "Search for new Higgs bosons via same-sign top quark pair production in association with a jet in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed and expected 95% CL upper limit on the signal strength as a function of $m_A$ for the g2HDM signal model using different coupling assumptions: $\rho_{tc}$ = 0.1, 0.4, 1.0.
description: No data abstract available.
DOI: 10.17182/hepdata.140528.v1/t7
title: "Figure 5a" of "Search for new Higgs bosons via same-sign top quark pair production in association with a jet in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed and expected 95% CL upper limit on the signal strength as a function of $m_A$ for the g2HDM signal model using different coupling assumptions: $\rho_{tu}$ = 0.1, 0.4, 1.0 with A–H interference assuming $m_A$ − $m_H$ = 50 GeV.
description: No data abstract available.
DOI: 10.17182/hepdata.140528.v1/t8
title: "Figure 5b" of "Search for new Higgs bosons via same-sign top quark pair production in association with a jet in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed and expected 95% CL upper limit on the signal strength as a function of $m_A$ for the g2HDM signal model using different coupling assumptions: $\rho_{tc}$ = 0.1, 0.4, 1.0 with A–H interference assuming $m_A$ − $m_H$ = 50 GeV.
description: No data abstract available.
DOI: 10.17182/hepdata.140528.v1/t9
title: "Figure 6a" of "Search for new Higgs bosons via same-sign top quark pair production in association with a jet in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed 95% CL upper limit on the signal strength as a function of $m_A$ and $\rho_{tu}$ for the g2HDM signal model.
description: No data abstract available.
DOI: 10.17182/hepdata.140528.v1/t12
title: "Figure 6b" of "Search for new Higgs bosons via same-sign top quark pair production in association with a jet in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed 95% CL upper limit on the signal strength as a function of $m_A$ and $\rho_{tc}$ for the g2HDM signal model.
description: No data abstract available.
DOI: 10.17182/hepdata.140528.v1/t13
title: "Figure 6b(expected exclusion)" of "Search for new Higgs bosons via same-sign top quark pair production in association with a jet in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected exclusion as a function of $m_A$ and $\rho_{tc}$ for the g2HDM signal model
description: No data abstract available.
DOI: 10.17182/hepdata.140528.v1/t14
title: "Figure 6b(observed exclusion)" of "Search for new Higgs bosons via same-sign top quark pair production in association with a jet in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed exclusion as a function of $m_A$ and $\rho_{tc}$ for the g2HDM signal model
description: No data abstract available.
DOI: 10.17182/hepdata.140528.v1/t15
title: "Figure 7a" of "Search for new Higgs bosons via same-sign top quark pair production in association with a jet in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed 95% CL upper limit on the signal strength as a function of $m_A$ and $\rho_{tu}$ for the g2HDM signal model with A–H interference assuming $m_A$ − $m_H$ = 50 GeV.
description: No data abstract available.
DOI: 10.17182/hepdata.140528.v1/t16
title: "Figure 7a(expected exclusion)" of "Search for new Higgs bosons via same-sign top quark pair production in association with a jet in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected exclusion as a function of $m_A$ and $\rho_{tu}$ for the g2HDM signal model with A–H interference assuming $m_A$ − $m_H$ = 50 GeV
description: No data abstract available.
DOI: 10.17182/hepdata.140528.v1/t17
title: "Figure 7a(observed exclusion)" of "Search for new Higgs bosons via same-sign top quark pair production in association with a jet in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed exclusion as a function of $m_A$ and $\rho_{tu}$ for the g2HDM signal model with A–H interference assuming $m_A$ − $m_H$ = 50 GeV
description: No data abstract available.
DOI: 10.17182/hepdata.140528.v1/t18
title: "Figure 7b" of "Search for new Higgs bosons via same-sign top quark pair production in association with a jet in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed 95% CL upper limit on the signal strength as a function of $m_A$ and $\rho_{tc}$ for the g2HDM signal model with A–H interference assuming $m_A$ − $m_H$ = 50 GeV.
description: No data abstract available.
DOI: 10.17182/hepdata.140528.v1/t19
title: "Figure 7b(expected exclusion)" of "Search for new Higgs bosons via same-sign top quark pair production in association with a jet in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected exclusion as a function of $m_A$ and $\rho_{tc}$ for the g2HDM signal model with A–H interference assuming $m_A$ − $m_H$ = 50 GeV
description: No data abstract available.
DOI: 10.17182/hepdata.140528.v1/t20
title: "Figure 7b(observed exclusion)" of "Search for new Higgs bosons via same-sign top quark pair production in association with a jet in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed exclusion as a function of $m_A$ and $\rho_{tc}$ for the g2HDM signal model with A–H interference assuming $m_A$ − $m_H$ = 50 GeV
description: No data abstract available.
DOI: 10.17182/hepdata.140529.v1/t1
title: "Figure 4a (Observed)" of "Combination and summary of ATLAS dark matter searches interpreted in a 2HDM with a pseudo-scalar mediator using 139 fb$^{-1}$ of $\sqrt{s} = 13$ TeV $pp$ collision data"

description: Observed combination limits at 95% CL in the $(m_{a},m_{A})$ plane under the assumption of $sin\theta$ = 0.35.
description: No data abstract available.
DOI: 10.17182/hepdata.140529.v1/t2
title: "Figure 4a (Expected)" of "Combination and summary of ATLAS dark matter searches interpreted in a 2HDM with a pseudo-scalar mediator using 139 fb$^{-1}$ of $\sqrt{s} = 13$ TeV $pp$ collision data"

description: Expected combination limits at 95% CL in the $(m_{a},m_{A})$ plane under the assumption of $sin\theta$ = 0.35.
description: No data abstract available.
DOI: 10.17182/hepdata.140529.v1/t3
title: "Figure 4a (Expected 1 sigma band)" of "Combination and summary of ATLAS dark matter searches interpreted in a 2HDM with a pseudo-scalar mediator using 139 fb$^{-1}$ of $\sqrt{s} = 13$ TeV $pp$ collision data"

description: 1 sigma band of expected combination limits at 95% CL in the $(m_{a},m_{A})$ plane under the assumption of $sin\theta$ = 0.35.
description: No data abstract available.
DOI: 10.17182/hepdata.140529.v1/t4
title: "Figure 4a (Expected 2 sigma band)" of "Combination and summary of ATLAS dark matter searches interpreted in a 2HDM with a pseudo-scalar mediator using 139 fb$^{-1}$ of $\sqrt{s} = 13$ TeV $pp$ collision data"

description: 2 sigma band of expected combination limits at 95% CL in the $(m_{a},m_{A})$ plane under the assumption of $sin\theta$ = 0.35.
description: No data abstract available.
DOI: 10.17182/hepdata.140529.v1/t5
title: "Figure 4b (Observed)" of "Combination and summary of ATLAS dark matter searches interpreted in a 2HDM with a pseudo-scalar mediator using 139 fb$^{-1}$ of $\sqrt{s} = 13$ TeV $pp$ collision data"

description: Observed combination limits at 95% CL in the $(m_{a},m_{A})$ plane under the assumption of $sin\theta$ = 0.7.
description: No data abstract available.