cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.76554.v1/t158
title: "Table 158" of "Measurement of differential cross sections for top quark pair production using the lepton+jets final state in proton-proton collisions at 13 TeV"

description: Normalized cross section at parton level.
description: Differential and double-differential cross sections for the production of top quark pairs in proton-proton collisions at 13 TeV are measured as a function of jet multiplicity and of kinematic variables of the top quarks and the top quark-antiquark system. This analysis is based on data collected by the CMS experiment at the LHC corresponding to an integrated luminosity of 2.3/fb. The measurements are performed in the lepton+jets decay channels with a single muon or electron in the final state. The differential cross sections are presented at particle level, within a phase space close to the experimental acceptance, and at parton level in the full phase space. The results are compared to several standard model predictions.
DOI: 10.17182/hepdata.76554.v1/t159
title: "Table 159" of "Measurement of differential cross sections for top quark pair production using the lepton+jets final state in proton-proton collisions at 13 TeV"

description: Covariance matrix of normalized cross section at parton level.
description: Differential and double-differential cross sections for the production of top quark pairs in proton-proton collisions at 13 TeV are measured as a function of jet multiplicity and of kinematic variables of the top quarks and the top quark-antiquark system. This analysis is based on data collected by the CMS experiment at the LHC corresponding to an integrated luminosity of 2.3/fb. The measurements are performed in the lepton+jets decay channels with a single muon or electron in the final state. The differential cross sections are presented at particle level, within a phase space close to the experimental acceptance, and at parton level in the full phase space. The results are compared to several standard model predictions.
DOI: 10.17182/hepdata.76554.v1/t160
title: "Table 160" of "Measurement of differential cross sections for top quark pair production using the lepton+jets final state in proton-proton collisions at 13 TeV"

description: Normalized cross section at parton level.
description: Differential and double-differential cross sections for the production of top quark pairs in proton-proton collisions at 13 TeV are measured as a function of jet multiplicity and of kinematic variables of the top quarks and the top quark-antiquark system. This analysis is based on data collected by the CMS experiment at the LHC corresponding to an integrated luminosity of 2.3/fb. The measurements are performed in the lepton+jets decay channels with a single muon or electron in the final state. The differential cross sections are presented at particle level, within a phase space close to the experimental acceptance, and at parton level in the full phase space. The results are compared to several standard model predictions.
DOI: 10.17182/hepdata.76554.v1/t161
title: "Table 161" of "Measurement of differential cross sections for top quark pair production using the lepton+jets final state in proton-proton collisions at 13 TeV"

description: Normalized cross section at parton level.
description: Differential and double-differential cross sections for the production of top quark pairs in proton-proton collisions at 13 TeV are measured as a function of jet multiplicity and of kinematic variables of the top quarks and the top quark-antiquark system. This analysis is based on data collected by the CMS experiment at the LHC corresponding to an integrated luminosity of 2.3/fb. The measurements are performed in the lepton+jets decay channels with a single muon or electron in the final state. The differential cross sections are presented at particle level, within a phase space close to the experimental acceptance, and at parton level in the full phase space. The results are compared to several standard model predictions.
DOI: 10.17182/hepdata.76554.v1/t162
title: "Table 162" of "Measurement of differential cross sections for top quark pair production using the lepton+jets final state in proton-proton collisions at 13 TeV"

description: Normalized cross section at parton level.
description: Differential and double-differential cross sections for the production of top quark pairs in proton-proton collisions at 13 TeV are measured as a function of jet multiplicity and of kinematic variables of the top quarks and the top quark-antiquark system. This analysis is based on data collected by the CMS experiment at the LHC corresponding to an integrated luminosity of 2.3/fb. The measurements are performed in the lepton+jets decay channels with a single muon or electron in the final state. The differential cross sections are presented at particle level, within a phase space close to the experimental acceptance, and at parton level in the full phase space. The results are compared to several standard model predictions.
DOI: 10.17182/hepdata.76554.v1/t163
title: "Table 163" of "Measurement of differential cross sections for top quark pair production using the lepton+jets final state in proton-proton collisions at 13 TeV"

description: Normalized cross section at parton level.
description: Differential and double-differential cross sections for the production of top quark pairs in proton-proton collisions at 13 TeV are measured as a function of jet multiplicity and of kinematic variables of the top quarks and the top quark-antiquark system. This analysis is based on data collected by the CMS experiment at the LHC corresponding to an integrated luminosity of 2.3/fb. The measurements are performed in the lepton+jets decay channels with a single muon or electron in the final state. The differential cross sections are presented at particle level, within a phase space close to the experimental acceptance, and at parton level in the full phase space. The results are compared to several standard model predictions.
DOI: 10.17182/hepdata.76554.v1/t164
title: "Table 164" of "Measurement of differential cross sections for top quark pair production using the lepton+jets final state in proton-proton collisions at 13 TeV"

description: Covariance matrix of normalized cross section at parton level.
description: Differential and double-differential cross sections for the production of top quark pairs in proton-proton collisions at 13 TeV are measured as a function of jet multiplicity and of kinematic variables of the top quarks and the top quark-antiquark system. This analysis is based on data collected by the CMS experiment at the LHC corresponding to an integrated luminosity of 2.3/fb. The measurements are performed in the lepton+jets decay channels with a single muon or electron in the final state. The differential cross sections are presented at particle level, within a phase space close to the experimental acceptance, and at parton level in the full phase space. The results are compared to several standard model predictions.
DOI: 10.17182/hepdata.76719.v1/t1
title: "Table 1" of "Measurement of the differential cross section of the reaction $\pi^+ d \rightarrow p p$ at medium energy"

description: No description provided.
description: No description provided.
DOI: 10.17182/hepdata.76722.v1/t1
title: "Table 1" of "On the construction of pion photoproduction amplitudes from experimental data"

description: '1'.
description: TECHNIQUE USED...ELECTRONIC.
DOI: 10.17182/hepdata.76722.v1/t2
title: "Table 2" of "On the construction of pion photoproduction amplitudes from experimental data"

description: '1'.
description: TECHNIQUE USED...ELECTRONIC.
DOI: 10.17182/hepdata.76722.v1/t3
title: "Table 3" of "On the construction of pion photoproduction amplitudes from experimental data"

description: '1'.
description: TECHNIQUE USED...ELECTRONIC.
DOI: 10.17182/hepdata.76727.v1/t1
title: "Table 1" of "Measurement of $R_{\text{uds}}$ and $R$ between 3.12 and 3.72 GeV at the KEDR detector"

description: Measured values of $R_{\rm{uds}}(s)$ and $R(s)$ with statistical and systematic uncertainties.
description: NOVOSIBIRSK-VEPP-4M. Using the KEDR detector at the VEPP-4M $e^+e^-$ collider, we have measured the values of $R_{\text{uds}}$ and $R$ at seven points of the center-of-mass energy between 3.12 and 3.72 GeV. The total achieved accuracy is about or better than $3.3\%$ at most of energy points with a systematic uncertainty of about $2.1\%$. At the moment it is the most accurate measurement of $R(s)$ in this energy range.
DOI: 10.17182/hepdata.76728.v1/t1
title: "Table 1" of "Search for triboson $W^{\pm}W^{\pm}W^{\mp}$ production in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector"

description: The measured fiducial and total cross sections. The first uncertainty is the statistical uncertainty, and the second one is the combine systematic uncertainty.
description: CERN-LHC. Measurements on the triboson W+-W+-W-+ production cross-section using two decay channels fully-leptonic W+-W+-W-+ -&gt; l+-nu l+-nu l-+nu and semi-leptonic W+-W+-W-+ -&gt; l+-nu l+-nu jj (with l=e,mu) in proton-proton collision data corresponding to an integrated luminosity of 20.3 fb-1 at a centre of-mass energy of 8 TeV with the ATLAS detector at the Large Hadron Collider. Limits are also sets on WWWW anomalous quartic gauge couplings.

The fully-leptonic channel (W+-W+-W-+ -&gt; l+-nu l+-nu l-+nu ) is defined as (the exact definition is given in table 1 of the preprint):
- Exactly 3 leptons electrons or muons with pT(Lepton)&gt;25 GeV and |eta(Leptons)|&lt;=2.5
- If there are 2 Same Flavor Opposite Signe (SFOS) pairs, MET&gt;55 GeV, if there is 1 SFOS, MET&gt;45 GeV, and if there is 0 SFOS pairs no requirement is applied on the MET.
- If there is no SFOS pairs the invariant mass between any lepton paires mll &gt; 20 GeV. No such requirements is applied in the presence of 1 or 2 SFOS pairs.
- The angle between the trilepton system and the pTMiss must be |phi_3l-phi_met|&gt;2.5
- If there is no SFOS pairs, |mee-mZ|&gt;15 GeV, if there is one SFOS pair mZ-mSFOS&gt;35 Gev or mSFOS-mZ&gt;25 GeV, and if there are two SFOS pairs mSFOS-mZ|&gt;20 GeV.
- There should be at most 1 jet with pT&gt;25 GeV and |eta|&lt;4.5


The semi-leptonic channel (W+-W+-W-+ -&gt; l+-nu l+-nu jj) is defined as (the exact definition is given in table 2 of the preprint):
- Exactly 2 same-charge leptons electrons or muons with pT(Lepton)&gt;30 GeV and |eta(Leptons)|&lt;=2.5
- Veto the presence of any third lepton with pT&gt;6 GeV and |\eta|&lt;2.5 GeV.
- In the ee final state mee&lt;80 GeV or mee&gt;100 GeV.
- The lepton pair should satisfy mll&gt;40 GeV.
- There should be at least 2 jets with pT(j1)&gt;30 GeV , pT(j2)&gt;30 GeV and |eta|&lt;2.5
- The dijet system should satisfy 65 GeV55 GeV.
DOI: 10.17182/hepdata.76728.v1/t2
title: "Table 2" of "Search for triboson $W^{\pm}W^{\pm}W^{\mp}$ production in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector"

description: 95% confidence level interval on FS0/lanbda^4 provided for different values of unitarity scale lambda_FF
description: CERN-LHC. Measurements on the triboson W+-W+-W-+ production cross-section using two decay channels fully-leptonic W+-W+-W-+ -&gt; l+-nu l+-nu l-+nu and semi-leptonic W+-W+-W-+ -&gt; l+-nu l+-nu jj (with l=e,mu) in proton-proton collision data corresponding to an integrated luminosity of 20.3 fb-1 at a centre of-mass energy of 8 TeV with the ATLAS detector at the Large Hadron Collider. Limits are also sets on WWWW anomalous quartic gauge couplings.

The fully-leptonic channel (W+-W+-W-+ -&gt; l+-nu l+-nu l-+nu ) is defined as (the exact definition is given in table 1 of the preprint):
- Exactly 3 leptons electrons or muons with pT(Lepton)&gt;25 GeV and |eta(Leptons)|&lt;=2.5
- If there are 2 Same Flavor Opposite Signe (SFOS) pairs, MET&gt;55 GeV, if there is 1 SFOS, MET&gt;45 GeV, and if there is 0 SFOS pairs no requirement is applied on the MET.
- If there is no SFOS pairs the invariant mass between any lepton paires mll &gt; 20 GeV. No such requirements is applied in the presence of 1 or 2 SFOS pairs.
- The angle between the trilepton system and the pTMiss must be |phi_3l-phi_met|&gt;2.5
- If there is no SFOS pairs, |mee-mZ|&gt;15 GeV, if there is one SFOS pair mZ-mSFOS&gt;35 Gev or mSFOS-mZ&gt;25 GeV, and if there are two SFOS pairs mSFOS-mZ|&gt;20 GeV.
- There should be at most 1 jet with pT&gt;25 GeV and |eta|&lt;4.5


The semi-leptonic channel (W+-W+-W-+ -&gt; l+-nu l+-nu jj) is defined as (the exact definition is given in table 2 of the preprint):
- Exactly 2 same-charge leptons electrons or muons with pT(Lepton)&gt;30 GeV and |eta(Leptons)|&lt;=2.5
- Veto the presence of any third lepton with pT&gt;6 GeV and |\eta|&lt;2.5 GeV.
- In the ee final state mee&lt;80 GeV or mee&gt;100 GeV.
- The lepton pair should satisfy mll&gt;40 GeV.
- There should be at least 2 jets with pT(j1)&gt;30 GeV , pT(j2)&gt;30 GeV and |eta|&lt;2.5
- The dijet system should satisfy 65 GeV55 GeV.
DOI: 10.17182/hepdata.76728.v1/t3
title: "Table 3" of "Search for triboson $W^{\pm}W^{\pm}W^{\mp}$ production in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector"

description: 95% confidence level interval on FS1/lanbda^4 provided for different values of unitarity scale lambda_FF
description: CERN-LHC. Measurements on the triboson W+-W+-W-+ production cross-section using two decay channels fully-leptonic W+-W+-W-+ -&gt; l+-nu l+-nu l-+nu and semi-leptonic W+-W+-W-+ -&gt; l+-nu l+-nu jj (with l=e,mu) in proton-proton collision data corresponding to an integrated luminosity of 20.3 fb-1 at a centre of-mass energy of 8 TeV with the ATLAS detector at the Large Hadron Collider. Limits are also sets on WWWW anomalous quartic gauge couplings.

The fully-leptonic channel (W+-W+-W-+ -&gt; l+-nu l+-nu l-+nu ) is defined as (the exact definition is given in table 1 of the preprint):
- Exactly 3 leptons electrons or muons with pT(Lepton)&gt;25 GeV and |eta(Leptons)|&lt;=2.5
- If there are 2 Same Flavor Opposite Signe (SFOS) pairs, MET&gt;55 GeV, if there is 1 SFOS, MET&gt;45 GeV, and if there is 0 SFOS pairs no requirement is applied on the MET.
- If there is no SFOS pairs the invariant mass between any lepton paires mll &gt; 20 GeV. No such requirements is applied in the presence of 1 or 2 SFOS pairs.
- The angle between the trilepton system and the pTMiss must be |phi_3l-phi_met|&gt;2.5
- If there is no SFOS pairs, |mee-mZ|&gt;15 GeV, if there is one SFOS pair mZ-mSFOS&gt;35 Gev or mSFOS-mZ&gt;25 GeV, and if there are two SFOS pairs mSFOS-mZ|&gt;20 GeV.
- There should be at most 1 jet with pT&gt;25 GeV and |eta|&lt;4.5


The semi-leptonic channel (W+-W+-W-+ -&gt; l+-nu l+-nu jj) is defined as (the exact definition is given in table 2 of the preprint):
- Exactly 2 same-charge leptons electrons or muons with pT(Lepton)&gt;30 GeV and |eta(Leptons)|&lt;=2.5
- Veto the presence of any third lepton with pT&gt;6 GeV and |\eta|&lt;2.5 GeV.
- In the ee final state mee&lt;80 GeV or mee&gt;100 GeV.
- The lepton pair should satisfy mll&gt;40 GeV.
- There should be at least 2 jets with pT(j1)&gt;30 GeV , pT(j2)&gt;30 GeV and |eta|&lt;2.5
- The dijet system should satisfy 65 GeV55 GeV.
DOI: 10.17182/hepdata.76728.v1/t4
title: "Table 4" of "Search for triboson $W^{\pm}W^{\pm}W^{\mp}$ production in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector"

description: 95% confidence level interval on alpha4 provided for different values of unitarity scale lambda_FF
description: CERN-LHC. Measurements on the triboson W+-W+-W-+ production cross-section using two decay channels fully-leptonic W+-W+-W-+ -&gt; l+-nu l+-nu l-+nu and semi-leptonic W+-W+-W-+ -&gt; l+-nu l+-nu jj (with l=e,mu) in proton-proton collision data corresponding to an integrated luminosity of 20.3 fb-1 at a centre of-mass energy of 8 TeV with the ATLAS detector at the Large Hadron Collider. Limits are also sets on WWWW anomalous quartic gauge couplings.

The fully-leptonic channel (W+-W+-W-+ -&gt; l+-nu l+-nu l-+nu ) is defined as (the exact definition is given in table 1 of the preprint):
- Exactly 3 leptons electrons or muons with pT(Lepton)&gt;25 GeV and |eta(Leptons)|&lt;=2.5
- If there are 2 Same Flavor Opposite Signe (SFOS) pairs, MET&gt;55 GeV, if there is 1 SFOS, MET&gt;45 GeV, and if there is 0 SFOS pairs no requirement is applied on the MET.
- If there is no SFOS pairs the invariant mass between any lepton paires mll &gt; 20 GeV. No such requirements is applied in the presence of 1 or 2 SFOS pairs.
- The angle between the trilepton system and the pTMiss must be |phi_3l-phi_met|&gt;2.5
- If there is no SFOS pairs, |mee-mZ|&gt;15 GeV, if there is one SFOS pair mZ-mSFOS&gt;35 Gev or mSFOS-mZ&gt;25 GeV, and if there are two SFOS pairs mSFOS-mZ|&gt;20 GeV.
- There should be at most 1 jet with pT&gt;25 GeV and |eta|&lt;4.5


The semi-leptonic channel (W+-W+-W-+ -&gt; l+-nu l+-nu jj) is defined as (the exact definition is given in table 2 of the preprint):
- Exactly 2 same-charge leptons electrons or muons with pT(Lepton)&gt;30 GeV and |eta(Leptons)|&lt;=2.5
- Veto the presence of any third lepton with pT&gt;6 GeV and |\eta|&lt;2.5 GeV.
- In the ee final state mee&lt;80 GeV or mee&gt;100 GeV.
- The lepton pair should satisfy mll&gt;40 GeV.
- There should be at least 2 jets with pT(j1)&gt;30 GeV , pT(j2)&gt;30 GeV and |eta|&lt;2.5
- The dijet system should satisfy 65 GeV55 GeV.
DOI: 10.17182/hepdata.76728.v1/t5
title: "Table 5" of "Search for triboson $W^{\pm}W^{\pm}W^{\mp}$ production in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector"

description: 95% confidence level interval on alpha5 provided for different values of unitarity scale lambda_FF
description: CERN-LHC. Measurements on the triboson W+-W+-W-+ production cross-section using two decay channels fully-leptonic W+-W+-W-+ -&gt; l+-nu l+-nu l-+nu and semi-leptonic W+-W+-W-+ -&gt; l+-nu l+-nu jj (with l=e,mu) in proton-proton collision data corresponding to an integrated luminosity of 20.3 fb-1 at a centre of-mass energy of 8 TeV with the ATLAS detector at the Large Hadron Collider. Limits are also sets on WWWW anomalous quartic gauge couplings.

The fully-leptonic channel (W+-W+-W-+ -&gt; l+-nu l+-nu l-+nu ) is defined as (the exact definition is given in table 1 of the preprint):
- Exactly 3 leptons electrons or muons with pT(Lepton)&gt;25 GeV and |eta(Leptons)|&lt;=2.5
- If there are 2 Same Flavor Opposite Signe (SFOS) pairs, MET&gt;55 GeV, if there is 1 SFOS, MET&gt;45 GeV, and if there is 0 SFOS pairs no requirement is applied on the MET.
- If there is no SFOS pairs the invariant mass between any lepton paires mll &gt; 20 GeV. No such requirements is applied in the presence of 1 or 2 SFOS pairs.
- The angle between the trilepton system and the pTMiss must be |phi_3l-phi_met|&gt;2.5
- If there is no SFOS pairs, |mee-mZ|&gt;15 GeV, if there is one SFOS pair mZ-mSFOS&gt;35 Gev or mSFOS-mZ&gt;25 GeV, and if there are two SFOS pairs mSFOS-mZ|&gt;20 GeV.
- There should be at most 1 jet with pT&gt;25 GeV and |eta|&lt;4.5


The semi-leptonic channel (W+-W+-W-+ -&gt; l+-nu l+-nu jj) is defined as (the exact definition is given in table 2 of the preprint):
- Exactly 2 same-charge leptons electrons or muons with pT(Lepton)&gt;30 GeV and |eta(Leptons)|&lt;=2.5
- Veto the presence of any third lepton with pT&gt;6 GeV and |\eta|&lt;2.5 GeV.
- In the ee final state mee&lt;80 GeV or mee&gt;100 GeV.
- The lepton pair should satisfy mll&gt;40 GeV.
- There should be at least 2 jets with pT(j1)&gt;30 GeV , pT(j2)&gt;30 GeV and |eta|&lt;2.5
- The dijet system should satisfy 65 GeV55 GeV.
DOI: 10.17182/hepdata.76728.v1/t7
title: "Table 7" of "Search for triboson $W^{\pm}W^{\pm}W^{\mp}$ production in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector"

description: A and C factors for each categories (ee, emu and mumu) of the semi-leptonic channel (W+-W+-W-+ -&gt; l+-nu l+-nu jj)
description: CERN-LHC. Measurements on the triboson W+-W+-W-+ production cross-section using two decay channels fully-leptonic W+-W+-W-+ -&gt; l+-nu l+-nu l-+nu and semi-leptonic W+-W+-W-+ -&gt; l+-nu l+-nu jj (with l=e,mu) in proton-proton collision data corresponding to an integrated luminosity of 20.3 fb-1 at a centre of-mass energy of 8 TeV with the ATLAS detector at the Large Hadron Collider. Limits are also sets on WWWW anomalous quartic gauge couplings.

The fully-leptonic channel (W+-W+-W-+ -&gt; l+-nu l+-nu l-+nu ) is defined as (the exact definition is given in table 1 of the preprint):
- Exactly 3 leptons electrons or muons with pT(Lepton)&gt;25 GeV and |eta(Leptons)|&lt;=2.5
- If there are 2 Same Flavor Opposite Signe (SFOS) pairs, MET&gt;55 GeV, if there is 1 SFOS, MET&gt;45 GeV, and if there is 0 SFOS pairs no requirement is applied on the MET.
- If there is no SFOS pairs the invariant mass between any lepton paires mll &gt; 20 GeV. No such requirements is applied in the presence of 1 or 2 SFOS pairs.
- The angle between the trilepton system and the pTMiss must be |phi_3l-phi_met|&gt;2.5
- If there is no SFOS pairs, |mee-mZ|&gt;15 GeV, if there is one SFOS pair mZ-mSFOS&gt;35 Gev or mSFOS-mZ&gt;25 GeV, and if there are two SFOS pairs mSFOS-mZ|&gt;20 GeV.
- There should be at most 1 jet with pT&gt;25 GeV and |eta|&lt;4.5


The semi-leptonic channel (W+-W+-W-+ -&gt; l+-nu l+-nu jj) is defined as (the exact definition is given in table 2 of the preprint):
- Exactly 2 same-charge leptons electrons or muons with pT(Lepton)&gt;30 GeV and |eta(Leptons)|&lt;=2.5
- Veto the presence of any third lepton with pT&gt;6 GeV and |\eta|&lt;2.5 GeV.
- In the ee final state mee&lt;80 GeV or mee&gt;100 GeV.
- The lepton pair should satisfy mll&gt;40 GeV.
- There should be at least 2 jets with pT(j1)&gt;30 GeV , pT(j2)&gt;30 GeV and |eta|&lt;2.5
- The dijet system should satisfy 65 GeV55 GeV.
DOI: 10.17182/hepdata.76728.v2/t1
title: "Table 1" of "Search for triboson $W^{\pm}W^{\pm}W^{\mp}$ production in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector"

description: The measured fiducial and total cross sections. The first uncertainty is the statistical uncertainty, and the second one is the combine systematic uncertainty.
description: CERN-LHC. Measurements on the triboson W+-W+-W-+ production cross-section using two decay channels fully-leptonic W+-W+-W-+ -&gt; l+-nu l+-nu l-+nu and semi-leptonic W+-W+-W-+ -&gt; l+-nu l+-nu jj (with l=e,mu) in proton-proton collision data corresponding to an integrated luminosity of 20.3 fb-1 at a centre of-mass energy of 8 TeV with the ATLAS detector at the Large Hadron Collider. Limits are also sets on WWWW anomalous quartic gauge couplings.

The fully-leptonic channel (W+-W+-W-+ -&gt; l+-nu l+-nu l-+nu ) is defined as (the exact definition is given in table 1 of the preprint):
- Exactly 3 leptons electrons or muons with pT(Lepton)&gt;25 GeV and |eta(Leptons)|&lt;=2.5
- If there are 2 Same Flavor Opposite Signe (SFOS) pairs, MET&gt;55 GeV, if there is 1 SFOS, MET&gt;45 GeV, and if there is 0 SFOS pairs no requirement is applied on the MET.
- If there is no SFOS pairs the invariant mass between any lepton paires mll &gt; 20 GeV. No such requirements is applied in the presence of 1 or 2 SFOS pairs.
- The angle between the trilepton system and the pTMiss must be |phi_3l-phi_met|&gt;2.5
- If there is no SFOS pairs, |mee-mZ|&gt;15 GeV, if there is one SFOS pair mZ-mSFOS&gt;35 Gev or mSFOS-mZ&gt;20 GeV, and if there are two SFOS pairs mSFOS-mZ|&gt;20 GeV.
- There should be at most 1 jet with pT&gt;25 GeV and |eta|&lt;4.5
- DeltaR(l,l)&gt;0.1


The semi-leptonic channel (W+-W+-W-+ -&gt; l+-nu l+-nu jj) is defined as (the exact definition is given in table 2 of the preprint):
- Exactly 2 same-charge leptons electrons or muons with pT(Lepton)&gt;30 GeV and |eta(Leptons)|&lt;=2.5
- Veto the presence of any third lepton with pT&gt;6 GeV and |\eta|&lt;2.5 GeV.
- In the ee final state mee&lt;80 GeV or mee&gt;100 GeV.
- The lepton pair should satisfy mll&gt;40 GeV.
- There should be at least 2 jets with pT(j1)&gt;30 GeV , pT(j2)&gt;30 GeV and |eta|&lt;2.5
- The dijet system should satisfy 65 GeV55 GeV.
- DeltaR(l,l)&gt;0.1 and DeltaR(l,j)&gt;0.3