cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.66933.v1/t6
title: "Table 6" of "Search for pair production of third-generation scalar leptoquarks and top squarks in proton-proton collisions at sqrt(s) = 8 TeV"

description: The final $S_{\text{T}}$ distribution for the top squark search with the $\text{e}\tau_{\text{h}}$ and $\mu\tau_{\text{h}}$ channels combined. The last bin contains the overflow events.
description: CERN-LHC. Search for pair production of third-generation scalar leptoquarks and top squarks in proton-proton collisions at $\sqrt{s}$ = 8 TeV using 19.7 inverse femtobarns of data collected with the CMS detector. The leptoquark search considers each leptoquark decaying to a tau lepton and a bottom quark, or each top squark decaying via an R-parity violating coupling $\lambda^{\prime}_{333}$ to a tau lepton and a bottom quark. The top squark search considers top squarks undergoing a chargino-mediated decay involving the R-parity violating coupling $\lambda^{\prime}_{3jk}$, each decaying to a tau lepton, a bottom quark, and two light quarks.

Errata:
17 JUN 2015: Fixed one typo from the paper: systematic uncertainties on the $M_{\text{LQ}}=700$ signal in Table 1 were a factor of ten too high.
17 JUN 2015: Fixed one typo just in the HepData entry: the $M_{\widetilde{\text{t}}}$ masses listed in Table 2 were incorrect.

Selection:
- one e/$\mu$ ($\ell$)
- e: $p_\text{T}$ &gt; 30 GeV, |$\eta$| &lt; 1.444 or 1.56 &lt; |$\eta$| &lt; 2.5
- $\mu$: $p_\text{T}$ &gt; 30 GeV, |$\eta$| &lt; 2.1
- one $\tau_{\text{h}}$ (hadronically decaying tau lepton): $p_\text{T}$ &gt; 50 GeV, |$\eta$| &lt; 2.3
- $\Delta$R($\ell$,$\tau_{\text{h}}$) &gt; 0.5; vertex($\ell$) = vertex($\tau_{\text{h}}$); charge($\ell$) != charge($\tau_{\text{h}}$)
- veto opposite sign $\mu$/e
- veto opposite sign e/$\mu$
- jet: $p_\text{T}$ &gt; 30 GeV, |$\eta$| &lt; 2.4
- $N_{\text{jet}}$ $\geq$ 2
- $N_{\text{b-jet}}$ $\geq$ 1
- $\Delta$R(jet,$\ell$) &gt; 0.5; $\Delta$R(jet,$\tau_{\text{h}}$) &gt; 0.5

Leptoquark search final selection:
- M($\tau_{\text{h}}$,jet) &gt; 250 GeV
(pairing is chosen that minimizes |M($\tau_{\text{h}}$,jet i) - M($\ell$,jet j)|)
- $S_{\text{T}}$ = $p_\text{T}$($\ell$) + $p_\text{T}$($\tau_{\text{h}}$) + $p_\text{T}$(b-jet) + $p_\text{T}$(jet)

Top squark search final selection:
- $N_\text{jet}$ $\geq$ 5
- $S_{\text{T}}$ = $p_\text{T}$($\ell$) + $p_\text{T}$($\tau_{\text{h}}$) + $p_\text{T}$(b-jet) + $p_\text{T}$(jet 1) + $p_\text{T}$(jet 2) + $p_\text{T}$(jet 3) + $p_\text{T}$(jet 4).
DOI: 10.15468/dl.d83nqt
title: Occurrence Download

description: A dataset containing 36907 species occurrences available in GBIF matching the query:
{
 "and" : [
 "TaxonKey is one of (Celastrus orbiculatus)",
 "HasCoordinate is true",
 "HasGeospatialIssue is false",
 "Year is greater than or equal to 1981",
 "OccurrenceStatus is Present",
 {
 "not" : {
 "BasisOfRecord" : [
 "is one of (Fossil, Living Specimen)"
 ]
 }
 },
 "Geometry POLYGON((-180 -90,180 -90,180 90,-180 90,-180 -90))"
 ]
}

 The dataset includes 36907 records from 231 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015301-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.66933.v1/t5
title: "Table 5" of "Search for pair production of third-generation scalar leptoquarks and top squarks in proton-proton collisions at sqrt(s) = 8 TeV"

description: The final $S_{\text{T}}$ distribution for the leptoquark search with the $\text{e}\tau_{\text{h}}$ and $\mu\tau_{\text{h}}$ channels combined. The last bin contains the overflow events.
description: CERN-LHC. Search for pair production of third-generation scalar leptoquarks and top squarks in proton-proton collisions at $\sqrt{s}$ = 8 TeV using 19.7 inverse femtobarns of data collected with the CMS detector. The leptoquark search considers each leptoquark decaying to a tau lepton and a bottom quark, or each top squark decaying via an R-parity violating coupling $\lambda^{\prime}_{333}$ to a tau lepton and a bottom quark. The top squark search considers top squarks undergoing a chargino-mediated decay involving the R-parity violating coupling $\lambda^{\prime}_{3jk}$, each decaying to a tau lepton, a bottom quark, and two light quarks.

Errata:
17 JUN 2015: Fixed one typo from the paper: systematic uncertainties on the $M_{\text{LQ}}=700$ signal in Table 1 were a factor of ten too high.
17 JUN 2015: Fixed one typo just in the HepData entry: the $M_{\widetilde{\text{t}}}$ masses listed in Table 2 were incorrect.

Selection:
- one e/$\mu$ ($\ell$)
- e: $p_\text{T}$ &gt; 30 GeV, |$\eta$| &lt; 1.444 or 1.56 &lt; |$\eta$| &lt; 2.5
- $\mu$: $p_\text{T}$ &gt; 30 GeV, |$\eta$| &lt; 2.1
- one $\tau_{\text{h}}$ (hadronically decaying tau lepton): $p_\text{T}$ &gt; 50 GeV, |$\eta$| &lt; 2.3
- $\Delta$R($\ell$,$\tau_{\text{h}}$) &gt; 0.5; vertex($\ell$) = vertex($\tau_{\text{h}}$); charge($\ell$) != charge($\tau_{\text{h}}$)
- veto opposite sign $\mu$/e
- veto opposite sign e/$\mu$
- jet: $p_\text{T}$ &gt; 30 GeV, |$\eta$| &lt; 2.4
- $N_{\text{jet}}$ $\geq$ 2
- $N_{\text{b-jet}}$ $\geq$ 1
- $\Delta$R(jet,$\ell$) &gt; 0.5; $\Delta$R(jet,$\tau_{\text{h}}$) &gt; 0.5

Leptoquark search final selection:
- M($\tau_{\text{h}}$,jet) &gt; 250 GeV
(pairing is chosen that minimizes |M($\tau_{\text{h}}$,jet i) - M($\ell$,jet j)|)
- $S_{\text{T}}$ = $p_\text{T}$($\ell$) + $p_\text{T}$($\tau_{\text{h}}$) + $p_\text{T}$(b-jet) + $p_\text{T}$(jet)

Top squark search final selection:
- $N_\text{jet}$ $\geq$ 5
- $S_{\text{T}}$ = $p_\text{T}$($\ell$) + $p_\text{T}$($\tau_{\text{h}}$) + $p_\text{T}$(b-jet) + $p_\text{T}$(jet 1) + $p_\text{T}$(jet 2) + $p_\text{T}$(jet 3) + $p_\text{T}$(jet 4).
DOI: 10.17182/hepdata.66933.v1/t7
title: "Table 7" of "Search for pair production of third-generation scalar leptoquarks and top squarks in proton-proton collisions at sqrt(s) = 8 TeV"

description: The expected and observed combined upper limits on the third-generation LQ pair production cross section $\sigma$ times the square of the branching fraction, $\mathcal{B}^2$, at 95% CL, as a function of the LQ mass. These limits also apply to top squarks decaying directly via the coupling $\lambda^{\prime}_{333}$.
description: CERN-LHC. Search for pair production of third-generation scalar leptoquarks and top squarks in proton-proton collisions at $\sqrt{s}$ = 8 TeV using 19.7 inverse femtobarns of data collected with the CMS detector. The leptoquark search considers each leptoquark decaying to a tau lepton and a bottom quark, or each top squark decaying via an R-parity violating coupling $\lambda^{\prime}_{333}$ to a tau lepton and a bottom quark. The top squark search considers top squarks undergoing a chargino-mediated decay involving the R-parity violating coupling $\lambda^{\prime}_{3jk}$, each decaying to a tau lepton, a bottom quark, and two light quarks.

Errata:
17 JUN 2015: Fixed one typo from the paper: systematic uncertainties on the $M_{\text{LQ}}=700$ signal in Table 1 were a factor of ten too high.
17 JUN 2015: Fixed one typo just in the HepData entry: the $M_{\widetilde{\text{t}}}$ masses listed in Table 2 were incorrect.

Selection:
- one e/$\mu$ ($\ell$)
- e: $p_\text{T}$ &gt; 30 GeV, |$\eta$| &lt; 1.444 or 1.56 &lt; |$\eta$| &lt; 2.5
- $\mu$: $p_\text{T}$ &gt; 30 GeV, |$\eta$| &lt; 2.1
- one $\tau_{\text{h}}$ (hadronically decaying tau lepton): $p_\text{T}$ &gt; 50 GeV, |$\eta$| &lt; 2.3
- $\Delta$R($\ell$,$\tau_{\text{h}}$) &gt; 0.5; vertex($\ell$) = vertex($\tau_{\text{h}}$); charge($\ell$) != charge($\tau_{\text{h}}$)
- veto opposite sign $\mu$/e
- veto opposite sign e/$\mu$
- jet: $p_\text{T}$ &gt; 30 GeV, |$\eta$| &lt; 2.4
- $N_{\text{jet}}$ $\geq$ 2
- $N_{\text{b-jet}}$ $\geq$ 1
- $\Delta$R(jet,$\ell$) &gt; 0.5; $\Delta$R(jet,$\tau_{\text{h}}$) &gt; 0.5

Leptoquark search final selection:
- M($\tau_{\text{h}}$,jet) &gt; 250 GeV
(pairing is chosen that minimizes |M($\tau_{\text{h}}$,jet i) - M($\ell$,jet j)|)
- $S_{\text{T}}$ = $p_\text{T}$($\ell$) + $p_\text{T}$($\tau_{\text{h}}$) + $p_\text{T}$(b-jet) + $p_\text{T}$(jet)

Top squark search final selection:
- $N_\text{jet}$ $\geq$ 5
- $S_{\text{T}}$ = $p_\text{T}$($\ell$) + $p_\text{T}$($\tau_{\text{h}}$) + $p_\text{T}$(b-jet) + $p_\text{T}$(jet 1) + $p_\text{T}$(jet 2) + $p_\text{T}$(jet 3) + $p_\text{T}$(jet 4).
DOI: 10.17182/hepdata.66933.v1/t8
title: "Table 8" of "Search for pair production of third-generation scalar leptoquarks and top squarks in proton-proton collisions at sqrt(s) = 8 TeV"

description: The expected and observed combined upper limits on the top squark pair production cross section $\sigma$ times the square of the branching fraction, $\mathcal{B}^2$, at 95% CL, as a function of the top squark mass. These limits apply to top squarks with a chargino-mediated decay through the coupling $\lambda^{\prime}_{3jk}$.
description: CERN-LHC. Search for pair production of third-generation scalar leptoquarks and top squarks in proton-proton collisions at $\sqrt{s}$ = 8 TeV using 19.7 inverse femtobarns of data collected with the CMS detector. The leptoquark search considers each leptoquark decaying to a tau lepton and a bottom quark, or each top squark decaying via an R-parity violating coupling $\lambda^{\prime}_{333}$ to a tau lepton and a bottom quark. The top squark search considers top squarks undergoing a chargino-mediated decay involving the R-parity violating coupling $\lambda^{\prime}_{3jk}$, each decaying to a tau lepton, a bottom quark, and two light quarks.

Errata:
17 JUN 2015: Fixed one typo from the paper: systematic uncertainties on the $M_{\text{LQ}}=700$ signal in Table 1 were a factor of ten too high.
17 JUN 2015: Fixed one typo just in the HepData entry: the $M_{\widetilde{\text{t}}}$ masses listed in Table 2 were incorrect.

Selection:
- one e/$\mu$ ($\ell$)
- e: $p_\text{T}$ &gt; 30 GeV, |$\eta$| &lt; 1.444 or 1.56 &lt; |$\eta$| &lt; 2.5
- $\mu$: $p_\text{T}$ &gt; 30 GeV, |$\eta$| &lt; 2.1
- one $\tau_{\text{h}}$ (hadronically decaying tau lepton): $p_\text{T}$ &gt; 50 GeV, |$\eta$| &lt; 2.3
- $\Delta$R($\ell$,$\tau_{\text{h}}$) &gt; 0.5; vertex($\ell$) = vertex($\tau_{\text{h}}$); charge($\ell$) != charge($\tau_{\text{h}}$)
- veto opposite sign $\mu$/e
- veto opposite sign e/$\mu$
- jet: $p_\text{T}$ &gt; 30 GeV, |$\eta$| &lt; 2.4
- $N_{\text{jet}}$ $\geq$ 2
- $N_{\text{b-jet}}$ $\geq$ 1
- $\Delta$R(jet,$\ell$) &gt; 0.5; $\Delta$R(jet,$\tau_{\text{h}}$) &gt; 0.5

Leptoquark search final selection:
- M($\tau_{\text{h}}$,jet) &gt; 250 GeV
(pairing is chosen that minimizes |M($\tau_{\text{h}}$,jet i) - M($\ell$,jet j)|)
- $S_{\text{T}}$ = $p_\text{T}$($\ell$) + $p_\text{T}$($\tau_{\text{h}}$) + $p_\text{T}$(b-jet) + $p_\text{T}$(jet)

Top squark search final selection:
- $N_\text{jet}$ $\geq$ 5
- $S_{\text{T}}$ = $p_\text{T}$($\ell$) + $p_\text{T}$($\tau_{\text{h}}$) + $p_\text{T}$(b-jet) + $p_\text{T}$(jet 1) + $p_\text{T}$(jet 2) + $p_\text{T}$(jet 3) + $p_\text{T}$(jet 4).
DOI: 10.17182/hepdata.66933.v1/t9
title: "Table 9" of "Search for pair production of third-generation scalar leptoquarks and top squarks in proton-proton collisions at sqrt(s) = 8 TeV"

description: The expected and observed 95% CL upper limits on the branching fraction for the leptoquark decay to a tau lepton and a bottom quark, as a function of the leptoquark mass. A search for top squark pair production [EPJC 73(2013)2677] has the same kinematic signature as the leptoquark decay to a tau neutrino and a top quark. This search is reinterpreted to provide the expected and observed 95% CL upper limits for low values of $\mathcal{B}$, assuming the leptoquark only decays to third-generation fermions.
description: CERN-LHC. Search for pair production of third-generation scalar leptoquarks and top squarks in proton-proton collisions at $\sqrt{s}$ = 8 TeV using 19.7 inverse femtobarns of data collected with the CMS detector. The leptoquark search considers each leptoquark decaying to a tau lepton and a bottom quark, or each top squark decaying via an R-parity violating coupling $\lambda^{\prime}_{333}$ to a tau lepton and a bottom quark. The top squark search considers top squarks undergoing a chargino-mediated decay involving the R-parity violating coupling $\lambda^{\prime}_{3jk}$, each decaying to a tau lepton, a bottom quark, and two light quarks.

Errata:
17 JUN 2015: Fixed one typo from the paper: systematic uncertainties on the $M_{\text{LQ}}=700$ signal in Table 1 were a factor of ten too high.
17 JUN 2015: Fixed one typo just in the HepData entry: the $M_{\widetilde{\text{t}}}$ masses listed in Table 2 were incorrect.

Selection:
- one e/$\mu$ ($\ell$)
- e: $p_\text{T}$ &gt; 30 GeV, |$\eta$| &lt; 1.444 or 1.56 &lt; |$\eta$| &lt; 2.5
- $\mu$: $p_\text{T}$ &gt; 30 GeV, |$\eta$| &lt; 2.1
- one $\tau_{\text{h}}$ (hadronically decaying tau lepton): $p_\text{T}$ &gt; 50 GeV, |$\eta$| &lt; 2.3
- $\Delta$R($\ell$,$\tau_{\text{h}}$) &gt; 0.5; vertex($\ell$) = vertex($\tau_{\text{h}}$); charge($\ell$) != charge($\tau_{\text{h}}$)
- veto opposite sign $\mu$/e
- veto opposite sign e/$\mu$
- jet: $p_\text{T}$ &gt; 30 GeV, |$\eta$| &lt; 2.4
- $N_{\text{jet}}$ $\geq$ 2
- $N_{\text{b-jet}}$ $\geq$ 1
- $\Delta$R(jet,$\ell$) &gt; 0.5; $\Delta$R(jet,$\tau_{\text{h}}$) &gt; 0.5

Leptoquark search final selection:
- M($\tau_{\text{h}}$,jet) &gt; 250 GeV
(pairing is chosen that minimizes |M($\tau_{\text{h}}$,jet i) - M($\ell$,jet j)|)
- $S_{\text{T}}$ = $p_\text{T}$($\ell$) + $p_\text{T}$($\tau_{\text{h}}$) + $p_\text{T}$(b-jet) + $p_\text{T}$(jet)

Top squark search final selection:
- $N_\text{jet}$ $\geq$ 5
- $S_{\text{T}}$ = $p_\text{T}$($\ell$) + $p_\text{T}$($\tau_{\text{h}}$) + $p_\text{T}$(b-jet) + $p_\text{T}$(jet 1) + $p_\text{T}$(jet 2) + $p_\text{T}$(jet 3) + $p_\text{T}$(jet 4).
DOI: 10.17182/hepdata.66985.v1/t1
title: "Table 1" of "Measurement of the Z gamma production cross section in pp collisions at 8 TeV and search for anomalous triple gauge boson couplings"

description: Inclusive fiducial cross sections in bins of pT(gamma) with statistical, systematic, and luminosity uncertainties, respectivley. Results are not divided by bin-widths. The last bin is the cross section for pT(gamma) &gt; 120 GeV. Combined result of electron and muon channels.
description: Measurement of the differential cross section for Zgamma production in proton-proton collisions at 8 TeV using a data sample of integrated luminosity of 19.5 fb-1 collected by the CMS experiment. The Z decay channels into muon and electron pairs are considered. The differential cross section as function of pT(gamma) is measured for a restricted phase space defined by:
- |eta(l)| &lt; 2.5, pT(l) &gt; 20 GeV
- Mass(ll) &gt; 50 GeV
- |eta(gamma)| &lt; 2.5 
- DeltaR(l, gamma) &gt; 0.7 
with l = muon,electron. In additon an isolation of less than 5 GeV in a cone of DeltaR = 0.3 around the photon is required. The cross section is measured inclusively and with a veto on jets where jets are reconstructed using the anti-kt algorithm with distance parameter DeltaR = 0.5. Only jets with pT &gt; 30 GeV and |eta| &lt; 2.4 are used for the veto. The cross sections are fully corrected for detector effects.
DOI: 10.17182/hepdata.66985.v1/t2
title: "Table 2" of "Measurement of the Z gamma production cross section in pp collisions at 8 TeV and search for anomalous triple gauge boson couplings"

description: Fiducial cross sections with jet-veto in bins of pT(gamma) with statistical, systematic, and luminosity uncertainties, respectivley. Results are not divided by bin-widths. The last bin is the cross section for pT(gamma) &gt; 120 GeV. Combined result of electron and muon channels.
description: Measurement of the differential cross section for Zgamma production in proton-proton collisions at 8 TeV using a data sample of integrated luminosity of 19.5 fb-1 collected by the CMS experiment. The Z decay channels into muon and electron pairs are considered. The differential cross section as function of pT(gamma) is measured for a restricted phase space defined by:
- |eta(l)| &lt; 2.5, pT(l) &gt; 20 GeV
- Mass(ll) &gt; 50 GeV
- |eta(gamma)| &lt; 2.5 
- DeltaR(l, gamma) &gt; 0.7 
with l = muon,electron. In additon an isolation of less than 5 GeV in a cone of DeltaR = 0.3 around the photon is required. The cross section is measured inclusively and with a veto on jets where jets are reconstructed using the anti-kt algorithm with distance parameter DeltaR = 0.5. Only jets with pT &gt; 30 GeV and |eta| &lt; 2.4 are used for the veto. The cross sections are fully corrected for detector effects.
DOI: 10.17182/hepdata.66985.v1/t3
title: "Table 3" of "Measurement of the Z gamma production cross section in pp collisions at 8 TeV and search for anomalous triple gauge boson couplings"

description: Ratio of fiducial cross section with jet-veto and the inclusive cross section in bins of pT(gamma). The last bin is the cross section for pT(gamma) &gt; 120 GeV. Combined result of electron and muon channels.
description: Measurement of the differential cross section for Zgamma production in proton-proton collisions at 8 TeV using a data sample of integrated luminosity of 19.5 fb-1 collected by the CMS experiment. The Z decay channels into muon and electron pairs are considered. The differential cross section as function of pT(gamma) is measured for a restricted phase space defined by:
- |eta(l)| &lt; 2.5, pT(l) &gt; 20 GeV
- Mass(ll) &gt; 50 GeV
- |eta(gamma)| &lt; 2.5 
- DeltaR(l, gamma) &gt; 0.7 
with l = muon,electron. In additon an isolation of less than 5 GeV in a cone of DeltaR = 0.3 around the photon is required. The cross section is measured inclusively and with a veto on jets where jets are reconstructed using the anti-kt algorithm with distance parameter DeltaR = 0.5. Only jets with pT &gt; 30 GeV and |eta| &lt; 2.4 are used for the veto. The cross sections are fully corrected for detector effects.
DOI: 10.17182/hepdata.66985.v1/t4
title: "Table 4" of "Measurement of the Z gamma production cross section in pp collisions at 8 TeV and search for anomalous triple gauge boson couplings"

description: Fiducial cross sections for pT(gamma) &gt; 15 GeV with statistical, systematic, and luminosity uncertainties, respectively. Combined result of electron and muon channels.
description: Measurement of the differential cross section for Zgamma production in proton-proton collisions at 8 TeV using a data sample of integrated luminosity of 19.5 fb-1 collected by the CMS experiment. The Z decay channels into muon and electron pairs are considered. The differential cross section as function of pT(gamma) is measured for a restricted phase space defined by:
- |eta(l)| &lt; 2.5, pT(l) &gt; 20 GeV
- Mass(ll) &gt; 50 GeV
- |eta(gamma)| &lt; 2.5 
- DeltaR(l, gamma) &gt; 0.7 
with l = muon,electron. In additon an isolation of less than 5 GeV in a cone of DeltaR = 0.3 around the photon is required. The cross section is measured inclusively and with a veto on jets where jets are reconstructed using the anti-kt algorithm with distance parameter DeltaR = 0.5. Only jets with pT &gt; 30 GeV and |eta| &lt; 2.4 are used for the veto. The cross sections are fully corrected for detector effects.
DOI: 10.17182/hepdata.66986.v1/t1
title: "Table 1" of "Search for squarks and gluinos in events with isolated leptons, jets and missing transverse momentum at $\sqrt{s}=8$ TeV with the ATLAS detector"

description: Observed and expected $E_T^{miss}/m_{eff}$ distribution in soft single-lepton 3-jet signal region. The last bin includes the overflow.
description: CERN-LHC. The results of a search for supersymmetry in final states containing at least one isolated lepton (electron or muon), jets and large missing transverse momentum with the ATLAS detector at the Large Hadron Collider (LHC) are reported. The search is based on proton-proton collision data at a centre-of-mass energy $\sqrt{s}=8$ TeV collected in 2012, corresponding to an integrated luminosity of 20 fb$^{-1}$. No significant excess above the Standard Model expectation is observed. Limits are set on the parameters of a minimal universal extra dimensions model, excluding a compactification radius of $1/R_{c}=950$ GeV for a cut-off scale times radius ($\Lambda R_{c}$) of approximately 30, as well as on sparticle masses for various supersymmetric models. Depending on the model, the search excludes gluino masses up to 1.32 TeV and squark masses up to 840 GeV.
DOI: 10.17182/hepdata.66986.v1/t2
title: "Table 2" of "Search for squarks and gluinos in events with isolated leptons, jets and missing transverse momentum at $\sqrt{s}=8$ TeV with the ATLAS detector"

description: Observed and expected $E_T^{miss}/m_{eff}$ distribution in soft single-lepton 5-jet signal region. The last bin includes the overflow.
description: CERN-LHC. The results of a search for supersymmetry in final states containing at least one isolated lepton (electron or muon), jets and large missing transverse momentum with the ATLAS detector at the Large Hadron Collider (LHC) are reported. The search is based on proton-proton collision data at a centre-of-mass energy $\sqrt{s}=8$ TeV collected in 2012, corresponding to an integrated luminosity of 20 fb$^{-1}$. No significant excess above the Standard Model expectation is observed. Limits are set on the parameters of a minimal universal extra dimensions model, excluding a compactification radius of $1/R_{c}=950$ GeV for a cut-off scale times radius ($\Lambda R_{c}$) of approximately 30, as well as on sparticle masses for various supersymmetric models. Depending on the model, the search excludes gluino masses up to 1.32 TeV and squark masses up to 840 GeV.
DOI: 10.17182/hepdata.66986.v1/t3
title: "Table 3" of "Search for squarks and gluinos in events with isolated leptons, jets and missing transverse momentum at $\sqrt{s}=8$ TeV with the ATLAS detector"

description: Observed and expected $E_T^{miss}/m_{eff}$ distribution in soft single-lepton 3-jet inclusive signal region. The last bin includes the overflow.
description: CERN-LHC. The results of a search for supersymmetry in final states containing at least one isolated lepton (electron or muon), jets and large missing transverse momentum with the ATLAS detector at the Large Hadron Collider (LHC) are reported. The search is based on proton-proton collision data at a centre-of-mass energy $\sqrt{s}=8$ TeV collected in 2012, corresponding to an integrated luminosity of 20 fb$^{-1}$. No significant excess above the Standard Model expectation is observed. Limits are set on the parameters of a minimal universal extra dimensions model, excluding a compactification radius of $1/R_{c}=950$ GeV for a cut-off scale times radius ($\Lambda R_{c}$) of approximately 30, as well as on sparticle masses for various supersymmetric models. Depending on the model, the search excludes gluino masses up to 1.32 TeV and squark masses up to 840 GeV.
DOI: 10.17182/hepdata.66986.v1/t4
title: "Table 4" of "Search for squarks and gluinos in events with isolated leptons, jets and missing transverse momentum at $\sqrt{s}=8$ TeV with the ATLAS detector"

description: Observed and expected $E_T^{miss}$ distribution in soft dimuon signal region. The last bin includes the overflow.
description: CERN-LHC. The results of a search for supersymmetry in final states containing at least one isolated lepton (electron or muon), jets and large missing transverse momentum with the ATLAS detector at the Large Hadron Collider (LHC) are reported. The search is based on proton-proton collision data at a centre-of-mass energy $\sqrt{s}=8$ TeV collected in 2012, corresponding to an integrated luminosity of 20 fb$^{-1}$. No significant excess above the Standard Model expectation is observed. Limits are set on the parameters of a minimal universal extra dimensions model, excluding a compactification radius of $1/R_{c}=950$ GeV for a cut-off scale times radius ($\Lambda R_{c}$) of approximately 30, as well as on sparticle masses for various supersymmetric models. Depending on the model, the search excludes gluino masses up to 1.32 TeV and squark masses up to 840 GeV.