cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.68759.v1/t4
title: "Table 4" of "Inclusive and differential measurements of the t t-bar charge asymmetry in pp collisions at sqrt(s) = 8 TeV"

description: Correlation matrix for the asymmetries as a function of $p_\text{T}^\mathrm{t\bar{t}}$ in the fiducial phase space. Both statistical and systematic effects are considered.
description: CERN-LHC. Measurements of the charge asymmetry in top quark production using the electron+jets and muon+jets decay channels in proton-proton collisions at a centre-of-mass energy of 8 TeV with 19.8/fb of data collected in 2012. Measurements are performed with extrapolations both to the full phase space or to a fiducial phase space.

The fiducial region is defined as:
- 4 particle-level jets of at least 30 GeV within $|\eta| &lt; 2.5$, clustered with the anti-kT algorithm with a resolution parameter of 0.5. Theoretical calculations should perform a clustering of the produced partons with the same parameters in order to emulate the particle-level jets used in the analysis.
- One electron or muon of $p_\text{T} &gt; 30 \, (27) \, \text{GeV}$ within $|\eta| &lt; 2.5 \,(2.1)$.
- Reject events with an additional electron or muon of $p_\text{T} &gt; 20 \, (10) \, \text{GeV}$ within $|\eta| &lt; 2.5 \,(2.5)$.
- Reject events where the axis of one of the clustered jets/partons has an angular separation of $\Delta R &lt; 0.4$ to the lepton, with $\Delta R = \sqrt{ (\Delta \eta)^2 + (\Delta \phi)^2 }$.
DOI: 10.17182/hepdata.68759.v1/t5
title: "Table 5" of "Inclusive and differential measurements of the t t-bar charge asymmetry in pp collisions at sqrt(s) = 8 TeV"

description: Corrected asymmetry as a function of $m_\mathrm{t\bar{t}}$ in the fiducial phase space, using three bins in $m_\mathrm{t\bar{t}}$. The value 9999 is used as a placeholder for infinity. The correlation matrix for these values can be found in a separate table.
description: CERN-LHC. Measurements of the charge asymmetry in top quark production using the electron+jets and muon+jets decay channels in proton-proton collisions at a centre-of-mass energy of 8 TeV with 19.8/fb of data collected in 2012. Measurements are performed with extrapolations both to the full phase space or to a fiducial phase space.

The fiducial region is defined as:
- 4 particle-level jets of at least 30 GeV within $|\eta| &lt; 2.5$, clustered with the anti-kT algorithm with a resolution parameter of 0.5. Theoretical calculations should perform a clustering of the produced partons with the same parameters in order to emulate the particle-level jets used in the analysis.
- One electron or muon of $p_\text{T} &gt; 30 \, (27) \, \text{GeV}$ within $|\eta| &lt; 2.5 \,(2.1)$.
- Reject events with an additional electron or muon of $p_\text{T} &gt; 20 \, (10) \, \text{GeV}$ within $|\eta| &lt; 2.5 \,(2.5)$.
- Reject events where the axis of one of the clustered jets/partons has an angular separation of $\Delta R &lt; 0.4$ to the lepton, with $\Delta R = \sqrt{ (\Delta \eta)^2 + (\Delta \phi)^2 }$.
DOI: 10.17182/hepdata.68759.v1/t10
title: "Table 10" of "Inclusive and differential measurements of the t t-bar charge asymmetry in pp collisions at sqrt(s) = 8 TeV"

description: Correlation matrix for the asymmetries as a function of $|y_\mathrm{t\bar{t}}|$ in the full phase space. Both statistical and systematic effects are considered.
description: CERN-LHC. Measurements of the charge asymmetry in top quark production using the electron+jets and muon+jets decay channels in proton-proton collisions at a centre-of-mass energy of 8 TeV with 19.8/fb of data collected in 2012. Measurements are performed with extrapolations both to the full phase space or to a fiducial phase space.

The fiducial region is defined as:
- 4 particle-level jets of at least 30 GeV within $|\eta| &lt; 2.5$, clustered with the anti-kT algorithm with a resolution parameter of 0.5. Theoretical calculations should perform a clustering of the produced partons with the same parameters in order to emulate the particle-level jets used in the analysis.
- One electron or muon of $p_\text{T} &gt; 30 \, (27) \, \text{GeV}$ within $|\eta| &lt; 2.5 \,(2.1)$.
- Reject events with an additional electron or muon of $p_\text{T} &gt; 20 \, (10) \, \text{GeV}$ within $|\eta| &lt; 2.5 \,(2.5)$.
- Reject events where the axis of one of the clustered jets/partons has an angular separation of $\Delta R &lt; 0.4$ to the lepton, with $\Delta R = \sqrt{ (\Delta \eta)^2 + (\Delta \phi)^2 }$.
DOI: 10.17182/hepdata.68759.v1/t11
title: "Table 11" of "Inclusive and differential measurements of the t t-bar charge asymmetry in pp collisions at sqrt(s) = 8 TeV"

description: Corrected asymmetry as a function of $p_\text{T}^\mathrm{t\bar{t}}$ in the full phase space. The value 9999 is used as a placeholder for infinity. The correlation matrix for these values can be found in a separate table.
description: CERN-LHC. Measurements of the charge asymmetry in top quark production using the electron+jets and muon+jets decay channels in proton-proton collisions at a centre-of-mass energy of 8 TeV with 19.8/fb of data collected in 2012. Measurements are performed with extrapolations both to the full phase space or to a fiducial phase space.

The fiducial region is defined as:
- 4 particle-level jets of at least 30 GeV within $|\eta| &lt; 2.5$, clustered with the anti-kT algorithm with a resolution parameter of 0.5. Theoretical calculations should perform a clustering of the produced partons with the same parameters in order to emulate the particle-level jets used in the analysis.
- One electron or muon of $p_\text{T} &gt; 30 \, (27) \, \text{GeV}$ within $|\eta| &lt; 2.5 \,(2.1)$.
- Reject events with an additional electron or muon of $p_\text{T} &gt; 20 \, (10) \, \text{GeV}$ within $|\eta| &lt; 2.5 \,(2.5)$.
- Reject events where the axis of one of the clustered jets/partons has an angular separation of $\Delta R &lt; 0.4$ to the lepton, with $\Delta R = \sqrt{ (\Delta \eta)^2 + (\Delta \phi)^2 }$.
DOI: 10.17182/hepdata.68759.v1/t6
title: "Table 6" of "Inclusive and differential measurements of the t t-bar charge asymmetry in pp collisions at sqrt(s) = 8 TeV"

description: Correlation matrix for the asymmetries as a function of $m_\mathrm{t\bar{t}}$ in the fiducial phase space, using three bins in $m_\mathrm{t\bar{t}}$. Both statistical and systematic effects are considered.
description: CERN-LHC. Measurements of the charge asymmetry in top quark production using the electron+jets and muon+jets decay channels in proton-proton collisions at a centre-of-mass energy of 8 TeV with 19.8/fb of data collected in 2012. Measurements are performed with extrapolations both to the full phase space or to a fiducial phase space.

The fiducial region is defined as:
- 4 particle-level jets of at least 30 GeV within $|\eta| &lt; 2.5$, clustered with the anti-kT algorithm with a resolution parameter of 0.5. Theoretical calculations should perform a clustering of the produced partons with the same parameters in order to emulate the particle-level jets used in the analysis.
- One electron or muon of $p_\text{T} &gt; 30 \, (27) \, \text{GeV}$ within $|\eta| &lt; 2.5 \,(2.1)$.
- Reject events with an additional electron or muon of $p_\text{T} &gt; 20 \, (10) \, \text{GeV}$ within $|\eta| &lt; 2.5 \,(2.5)$.
- Reject events where the axis of one of the clustered jets/partons has an angular separation of $\Delta R &lt; 0.4$ to the lepton, with $\Delta R = \sqrt{ (\Delta \eta)^2 + (\Delta \phi)^2 }$.
DOI: 10.17182/hepdata.68759.v1/t7
title: "Table 7" of "Inclusive and differential measurements of the t t-bar charge asymmetry in pp collisions at sqrt(s) = 8 TeV"

description: Corrected asymmetry as a function of $m_\mathrm{t\bar{t}}$ in the fiducial phase space, using six bins in $m_\mathrm{t\bar{t}}$. The value 9999 is used as a placeholder for infinity. The correlation matrix for these values can be found in a separate table.
description: CERN-LHC. Measurements of the charge asymmetry in top quark production using the electron+jets and muon+jets decay channels in proton-proton collisions at a centre-of-mass energy of 8 TeV with 19.8/fb of data collected in 2012. Measurements are performed with extrapolations both to the full phase space or to a fiducial phase space.

The fiducial region is defined as:
- 4 particle-level jets of at least 30 GeV within $|\eta| &lt; 2.5$, clustered with the anti-kT algorithm with a resolution parameter of 0.5. Theoretical calculations should perform a clustering of the produced partons with the same parameters in order to emulate the particle-level jets used in the analysis.
- One electron or muon of $p_\text{T} &gt; 30 \, (27) \, \text{GeV}$ within $|\eta| &lt; 2.5 \,(2.1)$.
- Reject events with an additional electron or muon of $p_\text{T} &gt; 20 \, (10) \, \text{GeV}$ within $|\eta| &lt; 2.5 \,(2.5)$.
- Reject events where the axis of one of the clustered jets/partons has an angular separation of $\Delta R &lt; 0.4$ to the lepton, with $\Delta R = \sqrt{ (\Delta \eta)^2 + (\Delta \phi)^2 }$.
DOI: 10.17182/hepdata.68759.v1/t8
title: "Table 8" of "Inclusive and differential measurements of the t t-bar charge asymmetry in pp collisions at sqrt(s) = 8 TeV"

description: Correlation matrix for the asymmetries as a function of $m_\mathrm{t\bar{t}}$ in the fiducial phase space, using six bins in $m_\mathrm{t\bar{t}}$. Both statistical and systematic effects are considered.
description: CERN-LHC. Measurements of the charge asymmetry in top quark production using the electron+jets and muon+jets decay channels in proton-proton collisions at a centre-of-mass energy of 8 TeV with 19.8/fb of data collected in 2012. Measurements are performed with extrapolations both to the full phase space or to a fiducial phase space.

The fiducial region is defined as:
- 4 particle-level jets of at least 30 GeV within $|\eta| &lt; 2.5$, clustered with the anti-kT algorithm with a resolution parameter of 0.5. Theoretical calculations should perform a clustering of the produced partons with the same parameters in order to emulate the particle-level jets used in the analysis.
- One electron or muon of $p_\text{T} &gt; 30 \, (27) \, \text{GeV}$ within $|\eta| &lt; 2.5 \,(2.1)$.
- Reject events with an additional electron or muon of $p_\text{T} &gt; 20 \, (10) \, \text{GeV}$ within $|\eta| &lt; 2.5 \,(2.5)$.
- Reject events where the axis of one of the clustered jets/partons has an angular separation of $\Delta R &lt; 0.4$ to the lepton, with $\Delta R = \sqrt{ (\Delta \eta)^2 + (\Delta \phi)^2 }$.
DOI: 10.17182/hepdata.68759.v1/t9
title: "Table 9" of "Inclusive and differential measurements of the t t-bar charge asymmetry in pp collisions at sqrt(s) = 8 TeV"

description: Corrected asymmetry as a function of $|y_\mathrm{t\bar{t}}|$ in the full phase space. The value 9999 is used as a placeholder for infinity. The correlation matrix for these values can be found in a separate table.
description: CERN-LHC. Measurements of the charge asymmetry in top quark production using the electron+jets and muon+jets decay channels in proton-proton collisions at a centre-of-mass energy of 8 TeV with 19.8/fb of data collected in 2012. Measurements are performed with extrapolations both to the full phase space or to a fiducial phase space.

The fiducial region is defined as:
- 4 particle-level jets of at least 30 GeV within $|\eta| &lt; 2.5$, clustered with the anti-kT algorithm with a resolution parameter of 0.5. Theoretical calculations should perform a clustering of the produced partons with the same parameters in order to emulate the particle-level jets used in the analysis.
- One electron or muon of $p_\text{T} &gt; 30 \, (27) \, \text{GeV}$ within $|\eta| &lt; 2.5 \,(2.1)$.
- Reject events with an additional electron or muon of $p_\text{T} &gt; 20 \, (10) \, \text{GeV}$ within $|\eta| &lt; 2.5 \,(2.5)$.
- Reject events where the axis of one of the clustered jets/partons has an angular separation of $\Delta R &lt; 0.4$ to the lepton, with $\Delta R = \sqrt{ (\Delta \eta)^2 + (\Delta \phi)^2 }$.
DOI: 10.17182/hepdata.68759.v1/t12
title: "Table 12" of "Inclusive and differential measurements of the t t-bar charge asymmetry in pp collisions at sqrt(s) = 8 TeV"

description: Correlation matrix for the asymmetries as a function of $p_\text{T}^\mathrm{t\bar{t}}$ in the full phase space. Both statistical and systematic effects are considered.
description: CERN-LHC. Measurements of the charge asymmetry in top quark production using the electron+jets and muon+jets decay channels in proton-proton collisions at a centre-of-mass energy of 8 TeV with 19.8/fb of data collected in 2012. Measurements are performed with extrapolations both to the full phase space or to a fiducial phase space.

The fiducial region is defined as:
- 4 particle-level jets of at least 30 GeV within $|\eta| &lt; 2.5$, clustered with the anti-kT algorithm with a resolution parameter of 0.5. Theoretical calculations should perform a clustering of the produced partons with the same parameters in order to emulate the particle-level jets used in the analysis.
- One electron or muon of $p_\text{T} &gt; 30 \, (27) \, \text{GeV}$ within $|\eta| &lt; 2.5 \,(2.1)$.
- Reject events with an additional electron or muon of $p_\text{T} &gt; 20 \, (10) \, \text{GeV}$ within $|\eta| &lt; 2.5 \,(2.5)$.
- Reject events where the axis of one of the clustered jets/partons has an angular separation of $\Delta R &lt; 0.4$ to the lepton, with $\Delta R = \sqrt{ (\Delta \eta)^2 + (\Delta \phi)^2 }$.
DOI: 10.17182/hepdata.68759.v1/t13
title: "Table 13" of "Inclusive and differential measurements of the t t-bar charge asymmetry in pp collisions at sqrt(s) = 8 TeV"

description: Corrected asymmetry as a function of $m_\mathrm{t\bar{t}}$ in the full phase space, using three bins in $m_\mathrm{t\bar{t}}$. The value 9999 is used as a placeholder for infinity. The correlation matrix for these values can be found in a separate table.
description: CERN-LHC. Measurements of the charge asymmetry in top quark production using the electron+jets and muon+jets decay channels in proton-proton collisions at a centre-of-mass energy of 8 TeV with 19.8/fb of data collected in 2012. Measurements are performed with extrapolations both to the full phase space or to a fiducial phase space.

The fiducial region is defined as:
- 4 particle-level jets of at least 30 GeV within $|\eta| &lt; 2.5$, clustered with the anti-kT algorithm with a resolution parameter of 0.5. Theoretical calculations should perform a clustering of the produced partons with the same parameters in order to emulate the particle-level jets used in the analysis.
- One electron or muon of $p_\text{T} &gt; 30 \, (27) \, \text{GeV}$ within $|\eta| &lt; 2.5 \,(2.1)$.
- Reject events with an additional electron or muon of $p_\text{T} &gt; 20 \, (10) \, \text{GeV}$ within $|\eta| &lt; 2.5 \,(2.5)$.
- Reject events where the axis of one of the clustered jets/partons has an angular separation of $\Delta R &lt; 0.4$ to the lepton, with $\Delta R = \sqrt{ (\Delta \eta)^2 + (\Delta \phi)^2 }$.
DOI: 10.17182/hepdata.68759.v1/t14
title: "Table 14" of "Inclusive and differential measurements of the t t-bar charge asymmetry in pp collisions at sqrt(s) = 8 TeV"

description: Correlation matrix for the asymmetries as a function of $m_\mathrm{t\bar{t}}$ in the full phase space, using three bins in $m_\mathrm{t\bar{t}}$. Both statistical and systematic effects are considered.
description: CERN-LHC. Measurements of the charge asymmetry in top quark production using the electron+jets and muon+jets decay channels in proton-proton collisions at a centre-of-mass energy of 8 TeV with 19.8/fb of data collected in 2012. Measurements are performed with extrapolations both to the full phase space or to a fiducial phase space.

The fiducial region is defined as:
- 4 particle-level jets of at least 30 GeV within $|\eta| &lt; 2.5$, clustered with the anti-kT algorithm with a resolution parameter of 0.5. Theoretical calculations should perform a clustering of the produced partons with the same parameters in order to emulate the particle-level jets used in the analysis.
- One electron or muon of $p_\text{T} &gt; 30 \, (27) \, \text{GeV}$ within $|\eta| &lt; 2.5 \,(2.1)$.
- Reject events with an additional electron or muon of $p_\text{T} &gt; 20 \, (10) \, \text{GeV}$ within $|\eta| &lt; 2.5 \,(2.5)$.
- Reject events where the axis of one of the clustered jets/partons has an angular separation of $\Delta R &lt; 0.4$ to the lepton, with $\Delta R = \sqrt{ (\Delta \eta)^2 + (\Delta \phi)^2 }$.
DOI: 10.17182/hepdata.68759.v1/t15
title: "Table 15" of "Inclusive and differential measurements of the t t-bar charge asymmetry in pp collisions at sqrt(s) = 8 TeV"

description: Corrected asymmetry as a function of $m_\mathrm{t\bar{t}}$ in the full phase space, using six bins in $m_\mathrm{t\bar{t}}$. The value 9999 is used as a placeholder for infinity. The correlation matrix for these values can be found in a separate table.
description: CERN-LHC. Measurements of the charge asymmetry in top quark production using the electron+jets and muon+jets decay channels in proton-proton collisions at a centre-of-mass energy of 8 TeV with 19.8/fb of data collected in 2012. Measurements are performed with extrapolations both to the full phase space or to a fiducial phase space.

The fiducial region is defined as:
- 4 particle-level jets of at least 30 GeV within $|\eta| &lt; 2.5$, clustered with the anti-kT algorithm with a resolution parameter of 0.5. Theoretical calculations should perform a clustering of the produced partons with the same parameters in order to emulate the particle-level jets used in the analysis.
- One electron or muon of $p_\text{T} &gt; 30 \, (27) \, \text{GeV}$ within $|\eta| &lt; 2.5 \,(2.1)$.
- Reject events with an additional electron or muon of $p_\text{T} &gt; 20 \, (10) \, \text{GeV}$ within $|\eta| &lt; 2.5 \,(2.5)$.
- Reject events where the axis of one of the clustered jets/partons has an angular separation of $\Delta R &lt; 0.4$ to the lepton, with $\Delta R = \sqrt{ (\Delta \eta)^2 + (\Delta \phi)^2 }$.
DOI: 10.17182/hepdata.68759.v1/t16
title: "Table 16" of "Inclusive and differential measurements of the t t-bar charge asymmetry in pp collisions at sqrt(s) = 8 TeV"

description: Correlation matrix for the asymmetries as a function of $m_\mathrm{t\bar{t}}$ in the full phase space, using six bins in $m_\mathrm{t\bar{t}}$. Both statistical and systematic effects are considered.
description: CERN-LHC. Measurements of the charge asymmetry in top quark production using the electron+jets and muon+jets decay channels in proton-proton collisions at a centre-of-mass energy of 8 TeV with 19.8/fb of data collected in 2012. Measurements are performed with extrapolations both to the full phase space or to a fiducial phase space.

The fiducial region is defined as:
- 4 particle-level jets of at least 30 GeV within $|\eta| &lt; 2.5$, clustered with the anti-kT algorithm with a resolution parameter of 0.5. Theoretical calculations should perform a clustering of the produced partons with the same parameters in order to emulate the particle-level jets used in the analysis.
- One electron or muon of $p_\text{T} &gt; 30 \, (27) \, \text{GeV}$ within $|\eta| &lt; 2.5 \,(2.1)$.
- Reject events with an additional electron or muon of $p_\text{T} &gt; 20 \, (10) \, \text{GeV}$ within $|\eta| &lt; 2.5 \,(2.5)$.
- Reject events where the axis of one of the clustered jets/partons has an angular separation of $\Delta R &lt; 0.4$ to the lepton, with $\Delta R = \sqrt{ (\Delta \eta)^2 + (\Delta \phi)^2 }$.
DOI: 10.17182/hepdata.68776.v1/t1
title: "Table 1" of "Search for quark contact interactions and extra spatial dimensions using dijet angular distributions in proton-proton collisions at sqrt(s) = 8 TeV"

description: Measured dijet angular distributions in bin of dijet invariant mass. P=3 and P=4 refers to the two jets in the final state.
description: CERN-LHC. Measurements of the dijet angular distribution in proton-proton collisions at a centre-of-mass energy of 8 TeV with 19.7 fb^-1 of data collected in 2012 by the CMS experiment.
DOI: 10.17182/hepdata.68776.v1/t2
title: "Table 2" of "Search for quark contact interactions and extra spatial dimensions using dijet angular distributions in proton-proton collisions at sqrt(s) = 8 TeV"

description: Measured dijet angular distributions in bin of dijet invariant mass.P=3 and P=4 refers to the two jets in the final state.
description: CERN-LHC. Measurements of the dijet angular distribution in proton-proton collisions at a centre-of-mass energy of 8 TeV with 19.7 fb^-1 of data collected in 2012 by the CMS experiment.
DOI: 10.17182/hepdata.68776.v1/t3
title: "Table 3" of "Search for quark contact interactions and extra spatial dimensions using dijet angular distributions in proton-proton collisions at sqrt(s) = 8 TeV"

description: Measured dijet angular distributions in bin of dijet invariant mass. P=3 and P=4 refers to the two jets in the final state.
description: CERN-LHC. Measurements of the dijet angular distribution in proton-proton collisions at a centre-of-mass energy of 8 TeV with 19.7 fb^-1 of data collected in 2012 by the CMS experiment.
DOI: 10.17182/hepdata.68776.v1/t4
title: "Table 4" of "Search for quark contact interactions and extra spatial dimensions using dijet angular distributions in proton-proton collisions at sqrt(s) = 8 TeV"

description: Measured dijet angular distributions in bin of dijet invariant mass. P=3 and P=4 refers to the two jets in the final state.
description: CERN-LHC. Measurements of the dijet angular distribution in proton-proton collisions at a centre-of-mass energy of 8 TeV with 19.7 fb^-1 of data collected in 2012 by the CMS experiment.
DOI: 10.17182/hepdata.68776.v1/t5
title: "Table 5" of "Search for quark contact interactions and extra spatial dimensions using dijet angular distributions in proton-proton collisions at sqrt(s) = 8 TeV"

description: Measured dijet angular distributions in bin of dijet invariant mass. P=3 and P=4 refers to the two jets in the final state.
description: CERN-LHC. Measurements of the dijet angular distribution in proton-proton collisions at a centre-of-mass energy of 8 TeV with 19.7 fb^-1 of data collected in 2012 by the CMS experiment.
DOI: 10.17182/hepdata.68777.v1/t1
title: "Table 1" of "Search for massive, long-lived particles using multitrack displaced vertices or displaced lepton pairs in pp collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector"

description: Vertex-level efficiency as a function of the vertex radial position for an RPV SUSY model of squark production with $\tilde{q}\to q[\tilde{\chi}_1^0\to\mu qq]$, where $m(\tilde{q}) = 700$ GeV, $m(\tilde{\chi}_1^0) = 494$ GeV and $c\tau(\tilde{\chi}_1^0)$ = 175 mm. This result is also represented in Figure 3b and Auxiliary Figure 1.
description: CERN-LHC. Many extensions of the Standard Model posit the existence of heavy particles with long lifetimes. This article presents the results of a search for events containing at least one long-lived particle that decays at a significant distance from its production point into two leptons or into five or more charged particles. This analysis uses a data sample of proton-proton collisions at $\sqrt{s}$ = 8 TeV corresponding to an integrated luminosity of 20.3 fb$^{-1}$ collected in 2012 by the ATLAS detector operating at the Large Hadron Collider. No events are observed in any of the signal regions, and limits are set on model parameters within supersymmetric scenarios involving R-parity violation, split supersymmetry, and gauge mediation. In some of the search channels, the trigger and search strategy are based only on the decay products of individual long-lived particles, irrespective of the rest of the event. In these cases, the provided limits can easily be reinterpreted in different scenarios.