cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.66352.v1/t2
title: "Table 2" 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 positively or negatively charged lepton pairs for various cuts on the dilepton invariant mass, $m(\ell \ell)$. 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.
DOI: 10.17182/hepdata.66352.v1/t4
title: "Table 4" 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: Lower limits at 95% CL on the mass of $H_{\mathrm{L}}^{\pm \pm}$ and $H_{\mathrm{R}}^{\pm \pm}$ bosons, assuming a 100% branching ratio to $e^{\pm}e^{\pm}$, $e^{\pm}/\mu^{\pm}$ and $\mu^{\pm}\mu^{\pm}$ pairs. The $1\sigma$ variations are also shown for the expected limits.
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.
DOI: 10.17898/adp_dzrs08_v1/1
title: dzrs08.tab

description: :unav
DOI: 10.17898/adp_dzrs08_v1/2
title: dzrs08_polna.tab

description: :unav
DOI: 10.17898/adp_dzrs08_v1
title: Vloga nacionalnega parlamenta v EU – primer Državnega zbora RS, 2008

description: Raziskava o stališčih poslancev o delovanju Državnega zbora RS daje vpogled v stališča poslancev glede nekaterih temeljnih elementov parlamentarizma v sodobnih liberalnih demokracijah. Na ta način se podrobneje opazuje percepcijo predstavništva interesov, ki predstavlja eno od temeljnih komponent poslanskega mandata, prav tako pa se opazuje celoten ustroj delovanja parlamenta z delovanjem delovnih teles na čelu. Cilj raziskave je odkriti, kako poslanci ocenjujejo delovanje in vidijo vlogo Državnega zbora RS v pogojih polnopravnega članstva v EU, ter kakšne so njihove predstave in pričakovanja glede možnosti vplivanja na sprejemanje odločitev in oblikovanje politik na ravni EU.
DOI: 10.17898/adp_dzrs08_v1/3
title: dzrs08.tab

description: :unav
DOI: 10.17182/hepdata.66358.v1/t1
title: "Table 1" of "Measurement of the production and lepton charge asymmetry of $\textit{W}$ bosons in Pb+Pb collisions at $\sqrt{s_{\mathrm{\mathbf{NN}}}}=$ 2.76 TeV with the ATLAS detector"

description: Ratio of W+ and W- candidates in $W\rightarrow \ell \nu_{\ell}$ as a function of the mean number of participants $N_{part}$.
description: CERN-LHC. A measurement of $\textit{W}$ boson production in lead-lead collisions at $\sqrt{s_{\mathrm{NN}}}=$2.76 TeV is presented. It is based on the analysis of data collected with the ATLAS detector at the LHC in 2011 corresponding to an integrated luminosity of 0.14 $\mathrm{nb}^{-1}$ and 0.15 $\mathrm{nb}^{-1}$ in the muon and electron decay channels, respectively. The differential production cross-sections and lepton charge asymmetry are each measured as a function of the average number of participating nucleons $\langle N_{\mathrm{part}} \rangle$ and absolute pseudorapidity of the charged lepton. The results are compared to predictions based on next-to-leading-order QCD calculations. These measurements are, in principle, sensitive to possible nuclear modifications to the parton distribution functions and also provide information on scaling of $\textit{W}$ boson production in multi-nucleon systems.
DOI: 10.17182/hepdata.66358.v1/t2
title: "Table 2" of "Measurement of the production and lepton charge asymmetry of $\textit{W}$ bosons in Pb+Pb collisions at $\sqrt{s_{\mathrm{\mathbf{NN}}}}=$ 2.76 TeV with the ATLAS detector"

description: $W^\pm$ boson production yield per binary collision as a function of the mean number of participants $N_{part}$.
description: CERN-LHC. A measurement of $\textit{W}$ boson production in lead-lead collisions at $\sqrt{s_{\mathrm{NN}}}=$2.76 TeV is presented. It is based on the analysis of data collected with the ATLAS detector at the LHC in 2011 corresponding to an integrated luminosity of 0.14 $\mathrm{nb}^{-1}$ and 0.15 $\mathrm{nb}^{-1}$ in the muon and electron decay channels, respectively. The differential production cross-sections and lepton charge asymmetry are each measured as a function of the average number of participating nucleons $\langle N_{\mathrm{part}} \rangle$ and absolute pseudorapidity of the charged lepton. The results are compared to predictions based on next-to-leading-order QCD calculations. These measurements are, in principle, sensitive to possible nuclear modifications to the parton distribution functions and also provide information on scaling of $\textit{W}$ boson production in multi-nucleon systems.
DOI: 10.17182/hepdata.66358.v1/t3
title: "Table 3" of "Measurement of the production and lepton charge asymmetry of $\textit{W}$ bosons in Pb+Pb collisions at $\sqrt{s_{\mathrm{\mathbf{NN}}}}=$ 2.76 TeV with the ATLAS detector"

description: Differential production yield per binary collision for $W^{+}$ bosons as a function of $|\eta_\ell|$.
description: CERN-LHC. A measurement of $\textit{W}$ boson production in lead-lead collisions at $\sqrt{s_{\mathrm{NN}}}=$2.76 TeV is presented. It is based on the analysis of data collected with the ATLAS detector at the LHC in 2011 corresponding to an integrated luminosity of 0.14 $\mathrm{nb}^{-1}$ and 0.15 $\mathrm{nb}^{-1}$ in the muon and electron decay channels, respectively. The differential production cross-sections and lepton charge asymmetry are each measured as a function of the average number of participating nucleons $\langle N_{\mathrm{part}} \rangle$ and absolute pseudorapidity of the charged lepton. The results are compared to predictions based on next-to-leading-order QCD calculations. These measurements are, in principle, sensitive to possible nuclear modifications to the parton distribution functions and also provide information on scaling of $\textit{W}$ boson production in multi-nucleon systems.
DOI: 10.17182/hepdata.66358.v1/t4
title: "Table 4" of "Measurement of the production and lepton charge asymmetry of $\textit{W}$ bosons in Pb+Pb collisions at $\sqrt{s_{\mathrm{\mathbf{NN}}}}=$ 2.76 TeV with the ATLAS detector"

description: Differential production yield per binary collision for $W^{-}$ bosons as a function of $|\eta_\ell|$.
description: CERN-LHC. A measurement of $\textit{W}$ boson production in lead-lead collisions at $\sqrt{s_{\mathrm{NN}}}=$2.76 TeV is presented. It is based on the analysis of data collected with the ATLAS detector at the LHC in 2011 corresponding to an integrated luminosity of 0.14 $\mathrm{nb}^{-1}$ and 0.15 $\mathrm{nb}^{-1}$ in the muon and electron decay channels, respectively. The differential production cross-sections and lepton charge asymmetry are each measured as a function of the average number of participating nucleons $\langle N_{\mathrm{part}} \rangle$ and absolute pseudorapidity of the charged lepton. The results are compared to predictions based on next-to-leading-order QCD calculations. These measurements are, in principle, sensitive to possible nuclear modifications to the parton distribution functions and also provide information on scaling of $\textit{W}$ boson production in multi-nucleon systems.
DOI: 10.17182/hepdata.66358.v1/t5
title: "Table 5" of "Measurement of the production and lepton charge asymmetry of $\textit{W}$ bosons in Pb+Pb collisions at $\sqrt{s_{\mathrm{\mathbf{NN}}}}=$ 2.76 TeV with the ATLAS detector"

description: The lepton charge asymmetry $A_{\ell}$ from $W^\pm$ bosons as a function of absolute pseudorapidity.
description: CERN-LHC. A measurement of $\textit{W}$ boson production in lead-lead collisions at $\sqrt{s_{\mathrm{NN}}}=$2.76 TeV is presented. It is based on the analysis of data collected with the ATLAS detector at the LHC in 2011 corresponding to an integrated luminosity of 0.14 $\mathrm{nb}^{-1}$ and 0.15 $\mathrm{nb}^{-1}$ in the muon and electron decay channels, respectively. The differential production cross-sections and lepton charge asymmetry are each measured as a function of the average number of participating nucleons $\langle N_{\mathrm{part}} \rangle$ and absolute pseudorapidity of the charged lepton. The results are compared to predictions based on next-to-leading-order QCD calculations. These measurements are, in principle, sensitive to possible nuclear modifications to the parton distribution functions and also provide information on scaling of $\textit{W}$ boson production in multi-nucleon systems.
DOI: 10.17182/hepdata.66456.v1/t1
title: "Table 1" of "Measurement of proton-proton elastic scattering and total cross-section at S**(1/2) = 7-TeV"

description: The measured differential elastic cross section.
description: CERN-LHC. Measurement of the elastic differential cross section in 
 proton-proton interactions at a centre-of-mass energy of 7 TeV. The data, 
 which cover the |t| range 0.005-0.2 GeV**2, were collected using Roman
 Pot detectors very close to the outgoing beam in October 2011, allowing
 the precise extrapolation down to the optical point, t=0, and hence the 
 derivation of the elastic as well as the total cross section via the 
 optical theorem. 
 An earler publication (CERN-PH-EP-2011-101,EPL 95(2011)41001) reports 
 measurements in the higher |t| range from 0.36-2.5 GeV**2.
DOI: 10.17182/hepdata.66456.v1/t2
title: "Table 2" of "Measurement of proton-proton elastic scattering and total cross-section at S**(1/2) = 7-TeV"

description: The measured differential elastic cross section in the high |T| region.

where it originally appeared as a plot, but was not tabulated.
description: CERN-LHC. Measurement of the elastic differential cross section in 
 proton-proton interactions at a centre-of-mass energy of 7 TeV. The data, 
 which cover the |t| range 0.005-0.2 GeV**2, were collected using Roman
 Pot detectors very close to the outgoing beam in October 2011, allowing
 the precise extrapolation down to the optical point, t=0, and hence the 
 derivation of the elastic as well as the total cross section via the 
 optical theorem. 
 An earler publication (CERN-PH-EP-2011-101,EPL 95(2011)41001) reports 
 measurements in the higher |t| range from 0.36-2.5 GeV**2.
DOI: 10.17182/hepdata.66456.v1/t3
title: "Table 3" of "Measurement of proton-proton elastic scattering and total cross-section at S**(1/2) = 7-TeV"

description: The fitted slope parameter for the elastic cross section fitted over 4 |T| ranges.
description: CERN-LHC. Measurement of the elastic differential cross section in 
 proton-proton interactions at a centre-of-mass energy of 7 TeV. The data, 
 which cover the |t| range 0.005-0.2 GeV**2, were collected using Roman
 Pot detectors very close to the outgoing beam in October 2011, allowing
 the precise extrapolation down to the optical point, t=0, and hence the 
 derivation of the elastic as well as the total cross section via the 
 optical theorem. 
 An earler publication (CERN-PH-EP-2011-101,EPL 95(2011)41001) reports 
 measurements in the higher |t| range from 0.36-2.5 GeV**2.
DOI: 10.17182/hepdata.66456.v1/t4
title: "Table 4" of "Measurement of proton-proton elastic scattering and total cross-section at S**(1/2) = 7-TeV"

description: The fitted elastic cross section parameters. The quoted systematic (sys) errors are from
the uncertainties in the T dependence, normalization and luminosity, respectively.:.
description: CERN-LHC. Measurement of the elastic differential cross section in 
 proton-proton interactions at a centre-of-mass energy of 7 TeV. The data, 
 which cover the |t| range 0.005-0.2 GeV**2, were collected using Roman
 Pot detectors very close to the outgoing beam in October 2011, allowing
 the precise extrapolation down to the optical point, t=0, and hence the 
 derivation of the elastic as well as the total cross section via the 
 optical theorem. 
 An earler publication (CERN-PH-EP-2011-101,EPL 95(2011)41001) reports 
 measurements in the higher |t| range from 0.36-2.5 GeV**2.
DOI: 10.17182/hepdata.66456.v1/t5
title: "Table 5" of "Measurement of proton-proton elastic scattering and total cross-section at S**(1/2) = 7-TeV"

description: The derived hadronic total and inelastic cross sections. The quoted systematic (sys) errors are from
the uncertainty in the T dependence, normalization, luminosity and rho (the ratio of the real/imaginary parts of the hadronic scattering
amplitude at T=0), respectively. The statistical errors are shown as zero:.
description: CERN-LHC. Measurement of the elastic differential cross section in 
 proton-proton interactions at a centre-of-mass energy of 7 TeV. The data, 
 which cover the |t| range 0.005-0.2 GeV**2, were collected using Roman
 Pot detectors very close to the outgoing beam in October 2011, allowing
 the precise extrapolation down to the optical point, t=0, and hence the 
 derivation of the elastic as well as the total cross section via the 
 optical theorem. 
 An earler publication (CERN-PH-EP-2011-101,EPL 95(2011)41001) reports 
 measurements in the higher |t| range from 0.36-2.5 GeV**2.
DOI: 10.17182/hepdata.66462.v1/t1
title: "Table 1" of "Searches for heavy long-lived charged particles with the ATLAS detector in proton-proton collisions at $\\sqrt{s}$ = 8 TeV"

description: Observed data, background estimate and expected signal in the slepton search for the lower of the two masses ($m$) in the two-candidate signal region (GMSB: $\tilde{\tau}_1$ masses of 344.5 and 437 GeV).
description: CERN-LHC. Searches for heavy long-lived charged particles are performed using a data sample of 19.8 fb$^{-1}$ from proton-proton collisions at a centre-of-mass energy of $\sqrt{s}$ = 8 TeV collected by the ATLAS detector at the Large Hadron Collider. No excess is observed above the estimated background and limits are placed on the mass of long-lived particles in various supersymmetric models. Long-lived tau sleptons in models with gauge-mediated symmetry breaking are excluded up to masses between 440 and 385 GeV for $\tan\beta$ between 10 and 50, with a 290 GeV limit in the case where only direct tau slepton production is considered. In the context of simplified LeptoSUSY models, where sleptons are stable and have a mass of 300 GeV, squark and gluino masses are excluded up to a mass of 1500 and 1360 GeV, respectively. Directly produced charginos, in simplified models where they are nearly degenerate to the lightest neutralino, are excluded up to a mass of 620 GeV. $R$-hadrons, composites containing a gluino, bottom squark or top squark, are excluded up to a mass of 1270, 845 and 900 GeV, respectively, using the full detector; and up to a mass of 1260, 835 and 870 GeV using an approach disregarding information from the muon spectrometer.
DOI: 10.17182/hepdata.66462.v1/t10
title: "Table 10" of "Searches for heavy long-lived charged particles with the ATLAS detector in proton-proton collisions at $\\sqrt{s}$ = 8 TeV"

description: Data and background estimates for the reconstructed mass based on specific energy loss, $m_{\beta\gamma}$, for the MS-agnostic 500 GeV stop R-Hadron search (SR-RH-MA).
description: CERN-LHC. Searches for heavy long-lived charged particles are performed using a data sample of 19.8 fb$^{-1}$ from proton-proton collisions at a centre-of-mass energy of $\sqrt{s}$ = 8 TeV collected by the ATLAS detector at the Large Hadron Collider. No excess is observed above the estimated background and limits are placed on the mass of long-lived particles in various supersymmetric models. Long-lived tau sleptons in models with gauge-mediated symmetry breaking are excluded up to masses between 440 and 385 GeV for $\tan\beta$ between 10 and 50, with a 290 GeV limit in the case where only direct tau slepton production is considered. In the context of simplified LeptoSUSY models, where sleptons are stable and have a mass of 300 GeV, squark and gluino masses are excluded up to a mass of 1500 and 1360 GeV, respectively. Directly produced charginos, in simplified models where they are nearly degenerate to the lightest neutralino, are excluded up to a mass of 620 GeV. $R$-hadrons, composites containing a gluino, bottom squark or top squark, are excluded up to a mass of 1270, 845 and 900 GeV, respectively, using the full detector; and up to a mass of 1260, 835 and 870 GeV using an approach disregarding information from the muon spectrometer.
DOI: 10.17182/hepdata.66462.v1/t2
title: "Table 2" of "Searches for heavy long-lived charged particles with the ATLAS detector in proton-proton collisions at $\\sqrt{s}$ = 8 TeV"

description: Observed data, background estimate and expected signal in the slepton search for the lower of the two masses ($m$) in the two-candidate signal region (GMSB: $\tilde{\tau}_1$ masses of 344.5 and 437 GeV).
description: CERN-LHC. Searches for heavy long-lived charged particles are performed using a data sample of 19.8 fb$^{-1}$ from proton-proton collisions at a centre-of-mass energy of $\sqrt{s}$ = 8 TeV collected by the ATLAS detector at the Large Hadron Collider. No excess is observed above the estimated background and limits are placed on the mass of long-lived particles in various supersymmetric models. Long-lived tau sleptons in models with gauge-mediated symmetry breaking are excluded up to masses between 440 and 385 GeV for $\tan\beta$ between 10 and 50, with a 290 GeV limit in the case where only direct tau slepton production is considered. In the context of simplified LeptoSUSY models, where sleptons are stable and have a mass of 300 GeV, squark and gluino masses are excluded up to a mass of 1500 and 1360 GeV, respectively. Directly produced charginos, in simplified models where they are nearly degenerate to the lightest neutralino, are excluded up to a mass of 620 GeV. $R$-hadrons, composites containing a gluino, bottom squark or top squark, are excluded up to a mass of 1270, 845 and 900 GeV, respectively, using the full detector; and up to a mass of 1260, 835 and 870 GeV using an approach disregarding information from the muon spectrometer.