cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.77382.v1/t20
title: "Table 19" of "Search for dark matter at $\sqrt{s}=13$ TeV in final states containing an energetic photon and large missing transverse momentum with the ATLAS detector"

description: The observed and expected 95% CL limits on M* for a dimension-7 operator EFT model with a contact interaction of type $\gamma\gamma\chi\chi$ as a function of dark-matter mass $m_{\chi}$.
description: CERN-LHC. Results of a search for physics beyond the Standard Model in events containing an energetic photon and large missing transverse momentum with the ATLAS detector at the Large Hadron Collider are reported. As the number of events observed in data, corresponding to an integrated luminosity of 36.1 fb$^{-1}$ of proton-proton collisions at a centre-of-mass energy of 13 TeV, is in agreement with the Standard Model expectations, exclusion limits in models where dark-matter candidates are pair-produced are determined. For dark-matter production via an axial-vector or a vector mediator in the s-channel, this search excludes mediator masses below 750-1200 GeV for dark-matter candidate masses below 230-480 GeV at 95% confidence level, depending on the couplings. In an effective theory of dark-matter production, the limits restrict the value of the suppression scale $M_{*}$ to be above 790 GeV at 95% confidence level. A limit is also reported on the production of a high-mass scalar resonance by processes beyond the Standard Model, in which the resonance decays to $Z\gamma$ and the $Z$ boson subsequently decays into neutrinos.
DOI: 10.17182/hepdata.77382.v1/t21
title: "Table 20" of "Search for dark matter at $\sqrt{s}=13$ TeV in final states containing an energetic photon and large missing transverse momentum with the ATLAS detector"

description: The observed and expected limit at 95% CL on the production cross section of a $Z\gamma$ resonance as a function of its mass.
description: CERN-LHC. Results of a search for physics beyond the Standard Model in events containing an energetic photon and large missing transverse momentum with the ATLAS detector at the Large Hadron Collider are reported. As the number of events observed in data, corresponding to an integrated luminosity of 36.1 fb$^{-1}$ of proton-proton collisions at a centre-of-mass energy of 13 TeV, is in agreement with the Standard Model expectations, exclusion limits in models where dark-matter candidates are pair-produced are determined. For dark-matter production via an axial-vector or a vector mediator in the s-channel, this search excludes mediator masses below 750-1200 GeV for dark-matter candidate masses below 230-480 GeV at 95% confidence level, depending on the couplings. In an effective theory of dark-matter production, the limits restrict the value of the suppression scale $M_{*}$ to be above 790 GeV at 95% confidence level. A limit is also reported on the production of a high-mass scalar resonance by processes beyond the Standard Model, in which the resonance decays to $Z\gamma$ and the $Z$ boson subsequently decays into neutrinos.
DOI: 10.17182/hepdata.77382.v1/t22
title: "Table 21" of "Search for dark matter at $\sqrt{s}=13$ TeV in final states containing an energetic photon and large missing transverse momentum with the ATLAS detector"

description: The observed 95% CL upper limits on signal strength $\mu$, the ratio of the experimental limit to the predicted signal cross section, for a simplified model of dark matter production involving an axial-vector operator, Dirac DM and couplings $g_{q}$ = 0.25 and $g_{\chi}$ = 1 as a function of the DM and the mediator particle masses. The bound on $\mu$ only applies for choices of couplings that yield the same kinematic distributions as the benchmark model.
description: CERN-LHC. Results of a search for physics beyond the Standard Model in events containing an energetic photon and large missing transverse momentum with the ATLAS detector at the Large Hadron Collider are reported. As the number of events observed in data, corresponding to an integrated luminosity of 36.1 fb$^{-1}$ of proton-proton collisions at a centre-of-mass energy of 13 TeV, is in agreement with the Standard Model expectations, exclusion limits in models where dark-matter candidates are pair-produced are determined. For dark-matter production via an axial-vector or a vector mediator in the s-channel, this search excludes mediator masses below 750-1200 GeV for dark-matter candidate masses below 230-480 GeV at 95% confidence level, depending on the couplings. In an effective theory of dark-matter production, the limits restrict the value of the suppression scale $M_{*}$ to be above 790 GeV at 95% confidence level. A limit is also reported on the production of a high-mass scalar resonance by processes beyond the Standard Model, in which the resonance decays to $Z\gamma$ and the $Z$ boson subsequently decays into neutrinos.
DOI: 10.17182/hepdata.77382.v1/t23
title: "Table 22" of "Search for dark matter at $\sqrt{s}=13$ TeV in final states containing an energetic photon and large missing transverse momentum with the ATLAS detector"

description: Acceptance, in %, for a simplified model of dark matter production involving an axial-vector operator, Dirac DM and couplings $g_{q}$= 0.25 and $g_{\chi}$ = 1 for various $m_{\chi}$ and $m_{\textrm{med}}$ values. It is constant as a function of $m_{\chi}$ for a fixed $m_{\textrm{med}}$ in the region $m_{\textrm{med}}&gt;2m_{\chi}$.
description: CERN-LHC. Results of a search for physics beyond the Standard Model in events containing an energetic photon and large missing transverse momentum with the ATLAS detector at the Large Hadron Collider are reported. As the number of events observed in data, corresponding to an integrated luminosity of 36.1 fb$^{-1}$ of proton-proton collisions at a centre-of-mass energy of 13 TeV, is in agreement with the Standard Model expectations, exclusion limits in models where dark-matter candidates are pair-produced are determined. For dark-matter production via an axial-vector or a vector mediator in the s-channel, this search excludes mediator masses below 750-1200 GeV for dark-matter candidate masses below 230-480 GeV at 95% confidence level, depending on the couplings. In an effective theory of dark-matter production, the limits restrict the value of the suppression scale $M_{*}$ to be above 790 GeV at 95% confidence level. A limit is also reported on the production of a high-mass scalar resonance by processes beyond the Standard Model, in which the resonance decays to $Z\gamma$ and the $Z$ boson subsequently decays into neutrinos.
DOI: 10.17182/hepdata.77382.v1/t24
title: "Table 23" of "Search for dark matter at $\sqrt{s}=13$ TeV in final states containing an energetic photon and large missing transverse momentum with the ATLAS detector"

description: Fiducial reconstruction efficiencies in the three inclusive signal regions for a simplified model of dark matter production involving an axial-vector operator, Dirac DM and couplings $g_{q}$= 0.25 and $g_{\chi}$ = 1 for various $m_{\chi}$ and $m_{\textrm{med}}$ values. It is constant as a function of $m_{\chi}$ for a fixed $m_{\textrm{med}}$ in the region $m_{\textrm{med}}&gt;2m_{\chi}$.
description: CERN-LHC. Results of a search for physics beyond the Standard Model in events containing an energetic photon and large missing transverse momentum with the ATLAS detector at the Large Hadron Collider are reported. As the number of events observed in data, corresponding to an integrated luminosity of 36.1 fb$^{-1}$ of proton-proton collisions at a centre-of-mass energy of 13 TeV, is in agreement with the Standard Model expectations, exclusion limits in models where dark-matter candidates are pair-produced are determined. For dark-matter production via an axial-vector or a vector mediator in the s-channel, this search excludes mediator masses below 750-1200 GeV for dark-matter candidate masses below 230-480 GeV at 95% confidence level, depending on the couplings. In an effective theory of dark-matter production, the limits restrict the value of the suppression scale $M_{*}$ to be above 790 GeV at 95% confidence level. A limit is also reported on the production of a high-mass scalar resonance by processes beyond the Standard Model, in which the resonance decays to $Z\gamma$ and the $Z$ boson subsequently decays into neutrinos.
DOI: 10.17182/hepdata.77426.v1/t1
title: "Table 1" of "Search for new physics with dijet angular distributions in proton-proton collisions at sqrt(s) = 13 TeV"

description: Normalized dijet angular distribution for events with dijet mass &gt; 4.8 TeV.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 2.6/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.77426.v2/t1
title: "Table 1" of "Search for new physics with dijet angular distributions in proton-proton collisions at sqrt(s) = 13 TeV"

description: Normalized dijet angular distribution for events with dijet mass &gt; 4.8 TeV.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 2.6/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.77426.v2/t2
title: "Table 2" of "Search for new physics with dijet angular distributions in proton-proton collisions at sqrt(s) = 13 TeV"

description: Normalized dijet angular distribution for events with 4.2 &lt; dijet mass &lt; 4.8 TeV.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 2.6/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.77426.v2/t3
title: "Table 3" of "Search for new physics with dijet angular distributions in proton-proton collisions at sqrt(s) = 13 TeV"

description: Normalized dijet angular distribution for events with 3.6 &lt; dijet mass &lt; 4.2 TeV.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 2.6/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.77426.v2/t4
title: "Table 4" of "Search for new physics with dijet angular distributions in proton-proton collisions at sqrt(s) = 13 TeV"

description: Normalized dijet angular distribution for events with 3.0 &lt; dijet mass &lt; 3.6 TeV.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 2.6/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.77426.v2/t5
title: "Table 5" of "Search for new physics with dijet angular distributions in proton-proton collisions at sqrt(s) = 13 TeV"

description: Normalized dijet angular distribution for events with 2.4 &lt; dijet mass &lt; 3.0 TeV.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 2.6/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.77426.v2/t6
title: "Table 6" of "Search for new physics with dijet angular distributions in proton-proton collisions at sqrt(s) = 13 TeV"

description: Normalized dijet angular distribution for events with 1.9 &lt; dijet mass &lt; 2.4 TeV.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 2.6/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.77426.v1/t2
title: "Table 2" of "Search for new physics with dijet angular distributions in proton-proton collisions at sqrt(s) = 13 TeV"

description: Normalized dijet angular distribution for events with 4.2 &lt; dijet mass &lt; 4.8 TeV.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 2.6/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.77426.v1/t3
title: "Table 3" of "Search for new physics with dijet angular distributions in proton-proton collisions at sqrt(s) = 13 TeV"

description: Normalized dijet angular distribution for events with 3.6 &lt; dijet mass &lt; 4.2 TeV.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 2.6/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.77426.v1/t4
title: "Table 4" of "Search for new physics with dijet angular distributions in proton-proton collisions at sqrt(s) = 13 TeV"

description: Normalized dijet angular distribution for events with 3.0 &lt; dijet mass &lt; 3.6 TeV.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 2.6/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.77426.v1/t5
title: "Table 5" of "Search for new physics with dijet angular distributions in proton-proton collisions at sqrt(s) = 13 TeV"

description: Normalized dijet angular distribution for events with 2.4 &lt; dijet mass &lt; 3.0 TeV.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 2.6/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.77426.v1/t6
title: "Table 6" of "Search for new physics with dijet angular distributions in proton-proton collisions at sqrt(s) = 13 TeV"

description: Normalized dijet angular distribution for events with 1.9 &lt; dijet mass &lt; 2.4 TeV.
description: CERN-LHC. Dijet angular distributions are measured in proton-proton collisions at sqrt(s)=13 TeV based on a data set corresponding to an integrated luminosity of 2.6/fb collected by the CMS detector at the CERN LHC.
DOI: 10.17182/hepdata.77436.v1/t1
title: "Figure 4a" of "Measurement of jet activity produced in top-quark events with an electron, a muon and two $b$-tagged jets in the final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Multiplicity of additional jets with pt&gt;25GeV
description: CERN-LHC, ATLAS. Measurement of jet activity in top-quark pair events produced in proton proton collisions at 13 TeV with 3.2fb-1 of data measured in 2015. Events are chosen by requiring an opposite-charge electron-muon pair and two b-tagged jets in the final state. Normalised differential cross sections are presented.
DOI: 10.17182/hepdata.77436.v1/t2
title: "Figure 4b" of "Measurement of jet activity produced in top-quark events with an electron, a muon and two $b$-tagged jets in the final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Multiplicity of additional jets with pt&gt;40GeV
description: CERN-LHC, ATLAS. Measurement of jet activity in top-quark pair events produced in proton proton collisions at 13 TeV with 3.2fb-1 of data measured in 2015. Events are chosen by requiring an opposite-charge electron-muon pair and two b-tagged jets in the final state. Normalised differential cross sections are presented.
DOI: 10.17182/hepdata.77436.v1/t3
title: "Figure 4c" of "Measurement of jet activity produced in top-quark events with an electron, a muon and two $b$-tagged jets in the final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Multiplicity of additional jets with pt&gt;60GeV
description: CERN-LHC, ATLAS. Measurement of jet activity in top-quark pair events produced in proton proton collisions at 13 TeV with 3.2fb-1 of data measured in 2015. Events are chosen by requiring an opposite-charge electron-muon pair and two b-tagged jets in the final state. Normalised differential cross sections are presented.
DOI: 10.17182/hepdata.77436.v1/t4
title: "Figure 4d" of "Measurement of jet activity produced in top-quark events with an electron, a muon and two $b$-tagged jets in the final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Multiplicity of additional jets with pt&gt;80GeV
description: CERN-LHC, ATLAS. Measurement of jet activity in top-quark pair events produced in proton proton collisions at 13 TeV with 3.2fb-1 of data measured in 2015. Events are chosen by requiring an opposite-charge electron-muon pair and two b-tagged jets in the final state. Normalised differential cross sections are presented.
DOI: 10.17182/hepdata.77436.v1/t5
title: "Figure 6a" of "Measurement of jet activity produced in top-quark events with an electron, a muon and two $b$-tagged jets in the final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Transverse momentum of leading b-jet
description: CERN-LHC, ATLAS. Measurement of jet activity in top-quark pair events produced in proton proton collisions at 13 TeV with 3.2fb-1 of data measured in 2015. Events are chosen by requiring an opposite-charge electron-muon pair and two b-tagged jets in the final state. Normalised differential cross sections are presented.
DOI: 10.17182/hepdata.77436.v1/t6
title: "Figure 6b" of "Measurement of jet activity produced in top-quark events with an electron, a muon and two $b$-tagged jets in the final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Transverse momentum of sub-leading b-jet
description: CERN-LHC, ATLAS. Measurement of jet activity in top-quark pair events produced in proton proton collisions at 13 TeV with 3.2fb-1 of data measured in 2015. Events are chosen by requiring an opposite-charge electron-muon pair and two b-tagged jets in the final state. Normalised differential cross sections are presented.
DOI: 10.17182/hepdata.77436.v1/t7
title: "Figure 6c" of "Measurement of jet activity produced in top-quark events with an electron, a muon and two $b$-tagged jets in the final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Transverse momentum of leading (highest pt) additional jet
description: CERN-LHC, ATLAS. Measurement of jet activity in top-quark pair events produced in proton proton collisions at 13 TeV with 3.2fb-1 of data measured in 2015. Events are chosen by requiring an opposite-charge electron-muon pair and two b-tagged jets in the final state. Normalised differential cross sections are presented.
DOI: 10.17182/hepdata.77436.v1/t10
title: "Figure 9c" of "Measurement of jet activity produced in top-quark events with an electron, a muon and two $b$-tagged jets in the final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Measured Gap fraction within 1.5&lt;|y|&lt;2.1 as a function of Q0
description: CERN-LHC, ATLAS. Measurement of jet activity in top-quark pair events produced in proton proton collisions at 13 TeV with 3.2fb-1 of data measured in 2015. Events are chosen by requiring an opposite-charge electron-muon pair and two b-tagged jets in the final state. Normalised differential cross sections are presented.
DOI: 10.17182/hepdata.77436.v1/t11
title: "Figure 9d" of "Measurement of jet activity produced in top-quark events with an electron, a muon and two $b$-tagged jets in the final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Measured Gap fraction within |y|&lt;2.1 as a function of Q0
description: CERN-LHC, ATLAS. Measurement of jet activity in top-quark pair events produced in proton proton collisions at 13 TeV with 3.2fb-1 of data measured in 2015. Events are chosen by requiring an opposite-charge electron-muon pair and two b-tagged jets in the final state. Normalised differential cross sections are presented.
DOI: 10.17182/hepdata.77436.v1/t13
title: "Figure 11b" of "Measurement of jet activity produced in top-quark events with an electron, a muon and two $b$-tagged jets in the final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Measured Gap fraction within 0.8&lt;|y|&lt;1.5 as a function of QSUM
description: CERN-LHC, ATLAS. Measurement of jet activity in top-quark pair events produced in proton proton collisions at 13 TeV with 3.2fb-1 of data measured in 2015. Events are chosen by requiring an opposite-charge electron-muon pair and two b-tagged jets in the final state. Normalised differential cross sections are presented.
DOI: 10.17182/hepdata.77436.v1/t14
title: "Figure 11c" of "Measurement of jet activity produced in top-quark events with an electron, a muon and two $b$-tagged jets in the final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Measured Gap fraction within 1.5&lt;|y|&lt;2.1 as a function of QSUM
description: CERN-LHC, ATLAS. Measurement of jet activity in top-quark pair events produced in proton proton collisions at 13 TeV with 3.2fb-1 of data measured in 2015. Events are chosen by requiring an opposite-charge electron-muon pair and two b-tagged jets in the final state. Normalised differential cross sections are presented.
DOI: 10.17182/hepdata.77436.v1/t8
title: "Figure 9a" of "Measurement of jet activity produced in top-quark events with an electron, a muon and two $b$-tagged jets in the final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Measured Gap fraction within |y|&lt;0.8 as a function of Q0
description: CERN-LHC, ATLAS. Measurement of jet activity in top-quark pair events produced in proton proton collisions at 13 TeV with 3.2fb-1 of data measured in 2015. Events are chosen by requiring an opposite-charge electron-muon pair and two b-tagged jets in the final state. Normalised differential cross sections are presented.
DOI: 10.17182/hepdata.77436.v1/t9
title: "Figure 9b" of "Measurement of jet activity produced in top-quark events with an electron, a muon and two $b$-tagged jets in the final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Measured Gap fraction within 0.8&lt;|y|&lt;1.5 as a function of Q0
description: CERN-LHC, ATLAS. Measurement of jet activity in top-quark pair events produced in proton proton collisions at 13 TeV with 3.2fb-1 of data measured in 2015. Events are chosen by requiring an opposite-charge electron-muon pair and two b-tagged jets in the final state. Normalised differential cross sections are presented.
DOI: 10.17182/hepdata.77436.v1/t12
title: "Figure 11a" of "Measurement of jet activity produced in top-quark events with an electron, a muon and two $b$-tagged jets in the final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Measured Gap fraction within |y|&lt;0.8 as a function of QSUM
description: CERN-LHC, ATLAS. Measurement of jet activity in top-quark pair events produced in proton proton collisions at 13 TeV with 3.2fb-1 of data measured in 2015. Events are chosen by requiring an opposite-charge electron-muon pair and two b-tagged jets in the final state. Normalised differential cross sections are presented.
DOI: 10.17182/hepdata.77436.v1/t15
title: "Figure 11d" of "Measurement of jet activity produced in top-quark events with an electron, a muon and two $b$-tagged jets in the final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Measured Gap fraction within |y|&lt;2.1 as a function of QSUM
description: CERN-LHC, ATLAS. Measurement of jet activity in top-quark pair events produced in proton proton collisions at 13 TeV with 3.2fb-1 of data measured in 2015. Events are chosen by requiring an opposite-charge electron-muon pair and two b-tagged jets in the final state. Normalised differential cross sections are presented.