cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.66280.v1/t3
title: "Table 3" of "Measurement of the muon charge asymmetry in ppbar to W + X to mu nu + X events at sqrt{s} = 1.96 TeV"

description: Contributions from individual sources of systematic uncertainty for the ($p^{\mu}_{T} &gt; 25$, $E_T^{missing} &gt; 25$) GeV kinematic region. 
All uncertainty values are multiplied by 100.
The columns (1-7) correspond to:
1.0 = Electro-Weak background
2.0 = Multi-Jet background
3.0 = Charge mis-identification
4.0 = Relative charge efficiency
5.0 = Magnet polarity weighting
6.0 = Momentum/$E_T^{missing}$ resolution
7.0 = Trigger isolation.
description: Fermilab-Tevatron. Measurement of the muon charge asymmetry from the decay of the $W$ boson via W to mu nu using 7.3 fb$^{-1}$ of integrated luminosity collected with the D0 detector at the Fermilab Tevatron Collider at sqrt(s) = 1.96 TeV. The muon charge asymmetry is presented in two kinematic regions in muon transverse momentum and event missing transverse energy: $(p^{\mu}_{T} &gt; 25$ GeV, $E_T^{missing} &gt; 25$ GeV) and $(p^{\mu}_{T} &gt; 35$ GeV, $E_T^{missing} &gt; 35$ GeV). The measured asymmetries are compared with theory predictions made using three parton distribution function sets. The predictions do not describe the data well for $p^{\mu}_{T} &gt; 35$ GeV, $E_T^{missing} &gt; 35$ GeV, and larger values of muon pseudorapidity.
DOI: 10.17182/hepdata.66280.v1/t4
title: "Table 4" of "Measurement of the muon charge asymmetry in ppbar to W + X to mu nu + X events at sqrt{s} = 1.96 TeV"

description: Contributions from individual sources of systematic uncertainty for the ($p^{\mu}_{T} &gt; 35$, $E_T^{missing} &gt; 35$) GeV kinematic region.
All uncertainty values are multiplied by 100.
The columns (1-7) correspond to:
1.0 = Electro-Weak background
2.0 = Multi-Jet background
3.0 = Charge mis-identification
4.0 = Relative charge efficiency
5.0 = Magnet polarity weighting
6.0 = Momentum/$E_T^{missing}$ resolution
7.0 = Trigger isolation.
description: Fermilab-Tevatron. Measurement of the muon charge asymmetry from the decay of the $W$ boson via W to mu nu using 7.3 fb$^{-1}$ of integrated luminosity collected with the D0 detector at the Fermilab Tevatron Collider at sqrt(s) = 1.96 TeV. The muon charge asymmetry is presented in two kinematic regions in muon transverse momentum and event missing transverse energy: $(p^{\mu}_{T} &gt; 25$ GeV, $E_T^{missing} &gt; 25$ GeV) and $(p^{\mu}_{T} &gt; 35$ GeV, $E_T^{missing} &gt; 35$ GeV). The measured asymmetries are compared with theory predictions made using three parton distribution function sets. The predictions do not describe the data well for $p^{\mu}_{T} &gt; 35$ GeV, $E_T^{missing} &gt; 35$ GeV, and larger values of muon pseudorapidity.
DOI: 10.17182/hepdata.66332.v1/t1
title: "Table 1" of "Event-by-event mean $p_{\rm T}$ fluctuations in pp and Pb-Pb collisions at the LHC"

description: Relative fluctuation $\sqrt{C_m}/M(p_{\rm T})_m$ as a function of $\langle {\rm d}N_{\rm ch}/{\rm d}\eta \rangle$ in pp collisions at $\sqrt{s}$ = 0.9 TeV.
description: CERN-LHC. Event-by-event fluctuations of the mean transverse momentum of charged particles produced in pp collisions at $\sqrt{s}$ = 0.9, 2.76 and 7 TeV, and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV are studied as a function of the charged-particle multiplicity using data measured in 2010 and 2011 by the ALICE detector at the LHC.
DOI: 10.17182/hepdata.66332.v1/t2
title: "Table 2" of "Event-by-event mean $p_{\rm T}$ fluctuations in pp and Pb-Pb collisions at the LHC"

description: Relative fluctuation $\sqrt{C_m}/M(p_{\rm T})_m$ as a function of $\langle {\rm d}N_{\rm ch}/{\rm d}\eta \rangle$ in pp collisions at $\sqrt{s}$ = 2.76 TeV.
description: CERN-LHC. Event-by-event fluctuations of the mean transverse momentum of charged particles produced in pp collisions at $\sqrt{s}$ = 0.9, 2.76 and 7 TeV, and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV are studied as a function of the charged-particle multiplicity using data measured in 2010 and 2011 by the ALICE detector at the LHC.
DOI: 10.17182/hepdata.66332.v1/t3
title: "Table 3" of "Event-by-event mean $p_{\rm T}$ fluctuations in pp and Pb-Pb collisions at the LHC"

description: Relative fluctuation $\sqrt{C_m}/M(p_{\rm T})_m$ as a function of $\langle {\rm d}N_{\rm ch}/{\rm d}\eta \rangle$ in pp collisions at $\sqrt{s}$ = 7 TeV.
description: CERN-LHC. Event-by-event fluctuations of the mean transverse momentum of charged particles produced in pp collisions at $\sqrt{s}$ = 0.9, 2.76 and 7 TeV, and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV are studied as a function of the charged-particle multiplicity using data measured in 2010 and 2011 by the ALICE detector at the LHC.
DOI: 10.17182/hepdata.66332.v1/t4
title: "Table 4" of "Event-by-event mean $p_{\rm T}$ fluctuations in pp and Pb-Pb collisions at the LHC"

description: Inclusive relative fluctuation $\sqrt{C}/M(p_{\rm T})$ as a function of $\sqrt{s}$ in pp collisions.
description: CERN-LHC. Event-by-event fluctuations of the mean transverse momentum of charged particles produced in pp collisions at $\sqrt{s}$ = 0.9, 2.76 and 7 TeV, and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV are studied as a function of the charged-particle multiplicity using data measured in 2010 and 2011 by the ALICE detector at the LHC.
DOI: 10.17182/hepdata.66332.v1/t5
title: "Table 5" of "Event-by-event mean $p_{\rm T}$ fluctuations in pp and Pb-Pb collisions at the LHC"

description: Relative fluctuation $\sqrt{C_m}/M(p_{\rm T})_m$ as a function of $\langle {\rm d}N_{\rm ch}/{\rm d}\eta \rangle$ in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV.
description: CERN-LHC. Event-by-event fluctuations of the mean transverse momentum of charged particles produced in pp collisions at $\sqrt{s}$ = 0.9, 2.76 and 7 TeV, and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV are studied as a function of the charged-particle multiplicity using data measured in 2010 and 2011 by the ALICE detector at the LHC.
DOI: 10.17182/hepdata.66332.v1/t6
title: "Table 6" of "Event-by-event mean $p_{\rm T}$ fluctuations in pp and Pb-Pb collisions at the LHC"

description: Relative fluctuation $\sqrt{C_m}/M(p_{\rm T})_m$ as a function of $\langle N_{\rm part} \rangle$ in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV.
description: CERN-LHC. Event-by-event fluctuations of the mean transverse momentum of charged particles produced in pp collisions at $\sqrt{s}$ = 0.9, 2.76 and 7 TeV, and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV are studied as a function of the charged-particle multiplicity using data measured in 2010 and 2011 by the ALICE detector at the LHC.
DOI: 10.17182/hepdata.66332.v1/t7
title: "Table 7" of "Event-by-event mean $p_{\rm T}$ fluctuations in pp and Pb-Pb collisions at the LHC"

description: Relative fluctuation $\sqrt{C_m}/M(p_{\rm T})_m$ normalized to $\langle {\rm d}N_{\rm ch}/{\rm d}\eta \rangle^{-0.5}$ as a function of $\langle {\rm d}N_{\rm ch}/{\rm d}\eta \rangle$ in pp collisions at $\sqrt{s}$ = 2.76 TeV.
description: CERN-LHC. Event-by-event fluctuations of the mean transverse momentum of charged particles produced in pp collisions at $\sqrt{s}$ = 0.9, 2.76 and 7 TeV, and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV are studied as a function of the charged-particle multiplicity using data measured in 2010 and 2011 by the ALICE detector at the LHC.
DOI: 10.17182/hepdata.66332.v1/t8
title: "Table 8" of "Event-by-event mean $p_{\rm T}$ fluctuations in pp and Pb-Pb collisions at the LHC"

description: Relative fluctuation $\sqrt{C_m}/M(p_{\rm T})_m$ normalized to $\langle {\rm d}N_{\rm ch}/{\rm d}\eta \rangle^{-0.5}$ as a function of $\langle {\rm d}N_{\rm ch}/{\rm d}\eta \rangle$ in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV.
description: CERN-LHC. Event-by-event fluctuations of the mean transverse momentum of charged particles produced in pp collisions at $\sqrt{s}$ = 0.9, 2.76 and 7 TeV, and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV are studied as a function of the charged-particle multiplicity using data measured in 2010 and 2011 by the ALICE detector at the LHC.
DOI: 10.17182/hepdata.66333.v1/t1
title: "Table 1" of "Measurement of the electron charge asymmetry in inclusive W production in pp collisions at sqrt(s) = 7 TeV"

description: Summary of the measured charge asymmetry results. The first uncertainty is statistical and the second is systematic. The theoretical predictions are obtained using MCFM interfaced with four different PDF models. The PDF uncertainties are estimated using the PDF reweighting technique. All values are in units of $10^{-3}$.
description: CERN-LHC. A measurement of the electron charge asymmetry in inclusive $pp \rightarrow W + X \rightarrow e \nu + X$ production at $\sqrt{s}$ = 7 TeV is presented based on data recorded by the CMS detector at the LHC and corresponding to an integrated luminosity of 840 pb$^{-1}$. The electron charge asymmetry reflects the unequal production of $W^+$ and $W^-$ bosons in $pp$ collisions. The electron charge asymmetry is measured in bins of absolute value of electron pseudorapidity in the range of $|\eta|$ &lt; 2.4. The asymmetry rises from about 0.1 to 0.2 as a function of the pseudorapidity and is measured with a relative precision better than 7%. This measurement provides new stringent constraints for parton distribution functions.
DOI: 10.17182/hepdata.66333.v1/t2
title: "Table 2" of "Measurement of the electron charge asymmetry in inclusive W production in pp collisions at sqrt(s) = 7 TeV"

description: Covariance matrix for the systematic uncertainties on the asymmetry. All values are given in units of $10^{-6}$.
description: CERN-LHC. A measurement of the electron charge asymmetry in inclusive $pp \rightarrow W + X \rightarrow e \nu + X$ production at $\sqrt{s}$ = 7 TeV is presented based on data recorded by the CMS detector at the LHC and corresponding to an integrated luminosity of 840 pb$^{-1}$. The electron charge asymmetry reflects the unequal production of $W^+$ and $W^-$ bosons in $pp$ collisions. The electron charge asymmetry is measured in bins of absolute value of electron pseudorapidity in the range of $|\eta|$ &lt; 2.4. The asymmetry rises from about 0.1 to 0.2 as a function of the pseudorapidity and is measured with a relative precision better than 7%. This measurement provides new stringent constraints for parton distribution functions.
DOI: 10.17182/hepdata.66344.v1/t1
title: "Table 1" of "Production of inclusive $\Upsilon$(1S) and $\Upsilon$(2S) in p-Pb collisions at $\mathbf{\sqrt{s_{{\rm NN}}} = 5.02}$ TeV"

description: Inclusive UPSI(1S) production cross section as a function of rapidity in p-Pb collisions at sqrt(s_NN) = 5.02 TeV. The data was collected in 2013 with two beam configurations, p-Pb and Pb-p with integrated luminosities of 5.0 nb-1 and 5.8 nb-1, respectively.
description: CERN-LHC. We report on the production of inclusive $\Upsilon(1S)$ and $\Upsilon(2S)$ in p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV at the LHC. 
The measurement is performed with the ALICE detector at backward ($-4.46 &lt; y_{{\rm cms}} &lt; -2.96$) and forward ($2.03 &lt; y_{{\rm cms}} &lt; 3.53$) rapidity down to zero transverse momentum. The production cross section of the $\Upsilon(1S)$ and $\Upsilon(2S)$ are presented, as well as the nuclear modification factor and the ratio of the forward to backward yields of $\Upsilon(1S)$. The data sets were taken in 2013 with two beam configurations, p-Pb and Pb-p with integrated luminosities of 5.0 nb-1 and 5.8 nb-1, respectively.
DOI: 10.17182/hepdata.66344.v1/t2
title: "Table 2" of "Production of inclusive $\Upsilon$(1S) and $\Upsilon$(2S) in p-Pb collisions at $\mathbf{\sqrt{s_{{\rm NN}}} = 5.02}$ TeV"

description: Inclusive UPSI(1S) production cross section as a function of rapidity in p-Pb collisions at sqrt(s_NN) = 5.02 TeV. The data was collected in 2013 with two beam configurations, p-Pb and Pb-p with integrated luminosities of 5.0 nb-1 and 5.8 nb-1, respectively.
description: CERN-LHC. We report on the production of inclusive $\Upsilon(1S)$ and $\Upsilon(2S)$ in p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV at the LHC. 
The measurement is performed with the ALICE detector at backward ($-4.46 &lt; y_{{\rm cms}} &lt; -2.96$) and forward ($2.03 &lt; y_{{\rm cms}} &lt; 3.53$) rapidity down to zero transverse momentum. The production cross section of the $\Upsilon(1S)$ and $\Upsilon(2S)$ are presented, as well as the nuclear modification factor and the ratio of the forward to backward yields of $\Upsilon(1S)$. The data sets were taken in 2013 with two beam configurations, p-Pb and Pb-p with integrated luminosities of 5.0 nb-1 and 5.8 nb-1, respectively.
DOI: 10.17182/hepdata.66344.v1/t3
title: "Table 3" of "Production of inclusive $\Upsilon$(1S) and $\Upsilon$(2S) in p-Pb collisions at $\mathbf{\sqrt{s_{{\rm NN}}} = 5.02}$ TeV"

description: Inclusive UPSI(2S) production cross section as a function of rapidity in p-Pb collisions at sqrt(s_NN) = 5.02 TeV. The data was collected in 2013 with two beam configurations, p-Pb and Pb-p with integrated luminosities of 5.0 nb-1 and 5.8 nb-1, respectively.
description: CERN-LHC. We report on the production of inclusive $\Upsilon(1S)$ and $\Upsilon(2S)$ in p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV at the LHC. 
The measurement is performed with the ALICE detector at backward ($-4.46 &lt; y_{{\rm cms}} &lt; -2.96$) and forward ($2.03 &lt; y_{{\rm cms}} &lt; 3.53$) rapidity down to zero transverse momentum. The production cross section of the $\Upsilon(1S)$ and $\Upsilon(2S)$ are presented, as well as the nuclear modification factor and the ratio of the forward to backward yields of $\Upsilon(1S)$. The data sets were taken in 2013 with two beam configurations, p-Pb and Pb-p with integrated luminosities of 5.0 nb-1 and 5.8 nb-1, respectively.
DOI: 10.17182/hepdata.66344.v1/t4
title: "Table 4" of "Production of inclusive $\Upsilon$(1S) and $\Upsilon$(2S) in p-Pb collisions at $\mathbf{\sqrt{s_{{\rm NN}}} = 5.02}$ TeV"

description: Nuclear modification factor of inclusive UPSI(1S) as a function of rapidity in p-Pb collisions at sqrt(s_NN) = 5.02 TeV. The data was collected in 2013 with two beam configurations, p-Pb and Pb-p with integrated luminosities of 5.0 nb-1 and 5.8 nb-1, respectively.
description: CERN-LHC. We report on the production of inclusive $\Upsilon(1S)$ and $\Upsilon(2S)$ in p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV at the LHC. 
The measurement is performed with the ALICE detector at backward ($-4.46 &lt; y_{{\rm cms}} &lt; -2.96$) and forward ($2.03 &lt; y_{{\rm cms}} &lt; 3.53$) rapidity down to zero transverse momentum. The production cross section of the $\Upsilon(1S)$ and $\Upsilon(2S)$ are presented, as well as the nuclear modification factor and the ratio of the forward to backward yields of $\Upsilon(1S)$. The data sets were taken in 2013 with two beam configurations, p-Pb and Pb-p with integrated luminosities of 5.0 nb-1 and 5.8 nb-1, respectively.
DOI: 10.17182/hepdata.66344.v1/t5
title: "Table 5" of "Production of inclusive $\Upsilon$(1S) and $\Upsilon$(2S) in p-Pb collisions at $\mathbf{\sqrt{s_{{\rm NN}}} = 5.02}$ TeV"

description: Nuclear modification factor of inclusive UPSI(1S) as a function of rapidity in p-Pb collisions at sqrt(sNN) = 5.02 TeV. The data was collected in 2013 with two beam configurations, p-Pb and Pb-p with integrated luminosities of 5.0 nb-1 and 5.8 nb-1, respectively.
description: CERN-LHC. We report on the production of inclusive $\Upsilon(1S)$ and $\Upsilon(2S)$ in p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV at the LHC. 
The measurement is performed with the ALICE detector at backward ($-4.46 &lt; y_{{\rm cms}} &lt; -2.96$) and forward ($2.03 &lt; y_{{\rm cms}} &lt; 3.53$) rapidity down to zero transverse momentum. The production cross section of the $\Upsilon(1S)$ and $\Upsilon(2S)$ are presented, as well as the nuclear modification factor and the ratio of the forward to backward yields of $\Upsilon(1S)$. The data sets were taken in 2013 with two beam configurations, p-Pb and Pb-p with integrated luminosities of 5.0 nb-1 and 5.8 nb-1, respectively.
DOI: 10.17182/hepdata.66344.v1/t6
title: "Table 6" of "Production of inclusive $\Upsilon$(1S) and $\Upsilon$(2S) in p-Pb collisions at $\mathbf{\sqrt{s_{{\rm NN}}} = 5.02}$ TeV"

description: Forward to backward ratio RFB of inclusive UPSI(1S) yields in p-Pb collisions at sqrt(sNN) = 5.02 TeV. The data was collected in 2013 with two beam configurations, p-Pb and Pb-p with integrated luminosities of 5.0 nb-1 and 5.8 nb-1, respectively.
description: CERN-LHC. We report on the production of inclusive $\Upsilon(1S)$ and $\Upsilon(2S)$ in p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV at the LHC. 
The measurement is performed with the ALICE detector at backward ($-4.46 &lt; y_{{\rm cms}} &lt; -2.96$) and forward ($2.03 &lt; y_{{\rm cms}} &lt; 3.53$) rapidity down to zero transverse momentum. The production cross section of the $\Upsilon(1S)$ and $\Upsilon(2S)$ are presented, as well as the nuclear modification factor and the ratio of the forward to backward yields of $\Upsilon(1S)$. The data sets were taken in 2013 with two beam configurations, p-Pb and Pb-p with integrated luminosities of 5.0 nb-1 and 5.8 nb-1, respectively.
DOI: 10.17182/hepdata.66344.v1/t7
title: "Table 7" of "Production of inclusive $\Upsilon$(1S) and $\Upsilon$(2S) in p-Pb collisions at $\mathbf{\sqrt{s_{{\rm NN}}} = 5.02}$ TeV"

description: Ratios of the cross sections of UPSI(2S)-&gt;MU+MU- to UPSI(1S)-&gt;MU+MU- in p-Pb collisions at sqrt(sNN) = 5.02 TeV. The data was collected in 2013 with two beam configurations, p-Pb and Pb-p with integrated luminosities of 5.0 nb-1 and 5.8 nb-1, respectively.
description: CERN-LHC. We report on the production of inclusive $\Upsilon(1S)$ and $\Upsilon(2S)$ in p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV at the LHC. 
The measurement is performed with the ALICE detector at backward ($-4.46 &lt; y_{{\rm cms}} &lt; -2.96$) and forward ($2.03 &lt; y_{{\rm cms}} &lt; 3.53$) rapidity down to zero transverse momentum. The production cross section of the $\Upsilon(1S)$ and $\Upsilon(2S)$ are presented, as well as the nuclear modification factor and the ratio of the forward to backward yields of $\Upsilon(1S)$. The data sets were taken in 2013 with two beam configurations, p-Pb and Pb-p with integrated luminosities of 5.0 nb-1 and 5.8 nb-1, respectively.
DOI: 10.17182/hepdata.66352.v1/t1
title: "Table 1" of "Search for anomalous production of prompt same-sign lepton pairs and pair-produced doubly charged Higgs bosons with $\sqrt{s} = 8$ TeV $pp$ collisions using the ATLAS detector"

description: Expected and observed numbers of isolated same-sign lepton pairs in the $e^{\pm}e^{\pm}, e^{\pm}\mu^{\pm}$ and $\mu^{\pm}\mu^{\pm}$ channel for various cuts on the dilepton invariant mass, m($\ell^{\pm}\ell^{\pm}$). The uncertainties shown are the systematic uncertainties.
description: CERN-LHC. A low-background inclusive search for new physics in events with same-sign dileptons is presented. The search uses proton-proton collisions corresponding to 20.3 fb$^{-1}$ of integrated luminosity taken in 2012 at a centre-of-mass energy of 8 TeV with the ATLAS detector at the LHC. Pairs of isolated leptons with the same electric charge and large transverse momenta of the type $e^{\pm}e^{\pm}, e^{\pm}\mu^{\pm}$, and $\mu^{\pm}\mu^{\pm}$ are selected and their invariant mass distribution is examined. No excess of events above the expected level of Standard Model background is found. The results are used to set upper limits on the cross sections for processes beyond the Standard Model. Limits are placed as a function of the dilepton invariant mass within a fiducial region corresponding to the signal event selection criteria. Exclusion limits are also derived for a specific model of doubly charged Higgs boson production.

The fiducial region in this analysis is defined as
- 2e, 2mu or emu
- both leptons have the same charge
- ptLepton(leading) &gt; 25 GeV; ptLepton(subleading) &gt; 20 GeV
- |etaLepton|&lt;2.5 for muons; |etaLepton|&lt;1.37 or 1.52 &lt; |etaLepton| &lt; 2.47 for electrons
- Sum pt of charged tracks in DeltaR=0.3 / ptLepton &lt; 0.07 for muons; Sum pt of charged tracks in DeltaR=0.3 / ptLepton &lt; 0.1 for electrons;
- same-sign lepton pari with mll &gt; 15 GeV
- mll excluded between 70 and 110 GeV for electrons
- no opposite-sign same-flavour pair with |mll-mZ| &lt; 10 GeV

To measure the fiducial efficiencies MC events are taken from the following processes
- doubly-charged Higgs (pair produced) with masses between 100 GeV and 1 TeV
- diquark (S$_{DQ}$) production with charge $\pm$ 2/3 or $\pm$ 4/3 in the Zee-Babu mode, which decay into 2 same-sign leptoquarks (S$_{LQ}$), decaying subsequently into a same-sign lepton pair. diquark masses between 2.5 TeV and 3.5 TeV and leptoquark masses between 1 TeV and 1.4 TeV are considered.
- Right-handed W$_R$ bosons decaying into a lepton and a Majorana neutrino N$_R$, with N$_R$ subsequently decaying into a lepton and two jets, for W$_R$ masses between 1 TeV and 2 TeV, and N$_R$ masses between 250 GeV and 1.5 TeV.
- Pair production of $b\prime$ chiral quarks, decaying either exclusively into Wt or decaying into Wq, q being an up-type quark, with a 33% branching ratio in each quark channel, for $b\prime$ masses between 400 GeV and 1 TeV.
The lowest fiducial efficiency, which is subsequently used in the limits, is 48%, 50% and 46% in the $e^{\pm}e^{\pm}, e^{\pm}\mu^{\pm}$ and $\mu^{\pm}\mu^{\pm}$ channel respectively.