cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.64435.v1/t37
title: "Table 37" of "Search for Anomalous Production of Events with Three or More Leptons in $pp$ Collisions at $\sqrt{s} =$ 8 TeV"

description: Observed 95% C.L. limits on BR(NEUTRALINO1 --&gt; HIGGS GRAVITINO) for the natural Higgsino NLSP scenario with fixed chargino-Higgsino mass of 250 GeV assuming BR(NEUTRALINO1 --&gt; HIGGS GRAVITINO) + BR(NEUTRALINO1 --&gt; Z GRAVITINO) = 1.0 and strong plus weak production.
description: CERN-LHC. A search for physics beyond the standard model in events with at least three leptons is presented. The data sample, corresponding to an integrated luminosity of 19.5 inverse femtobarns of proton-proton collisions with center-of-mass energy sqrt(s) = 8 TeV, was collected by the CMS experiment at the LHC during 2012. The data are divided into exclusive categories based on the number of leptons and their flavor, the presence or absence of an opposite-sign, same-flavor lepton pair (OSSF), the invariant mass of the OSSF pair, the presence or absence of a tagged bottom-quark jet, the number of identified hadronically decaying tau leptons, and the magnitude of the missing transverse energy and of the scalar sum of jet transverse momenta. 

We also place a 95% confidence level upper limit of 1.3% on the branching fraction for the decay of a top quark to a charm quark and a Higgs boson (TOP --&gt; CHARM HIGGS), which translates to a bound on the left- and right-handed top-charm flavor-violating Higgs Yukawa couplings, LAMBDA(HIGGS TOP CHARM) and LAMBDA(HIGGS CHARM TOP) respectively, of SQRT(ABS(LAMBDA(HIGGS TOP CHARM))**2 + ABS(LAMBDA(HIGGS CHARM TOP))**2) &lt; 0.21. 

We also present the product of the acceptance and efficiency for the calculations of the 95% C.L. in several different SUSY scenarios.
DOI: 10.17182/hepdata.64435.v1/t38
title: "Table 38" of "Search for Anomalous Production of Events with Three or More Leptons in $pp$ Collisions at $\sqrt{s} =$ 8 TeV"

description: Observed 95% C.L. limits on BR(NEUTRALINO1 --&gt; HIGGS GRAVITINO) for the natural Higgsino NLSP scenario with fixed chargino-Higgsino mass of 350 GeV assuming BR(NEUTRALINO1 --&gt; HIGGS GRAVITINO) + BR(NEUTRALINO1 --&gt; Z GRAVITINO) = 1.0 and strong plus weak production.
description: CERN-LHC. A search for physics beyond the standard model in events with at least three leptons is presented. The data sample, corresponding to an integrated luminosity of 19.5 inverse femtobarns of proton-proton collisions with center-of-mass energy sqrt(s) = 8 TeV, was collected by the CMS experiment at the LHC during 2012. The data are divided into exclusive categories based on the number of leptons and their flavor, the presence or absence of an opposite-sign, same-flavor lepton pair (OSSF), the invariant mass of the OSSF pair, the presence or absence of a tagged bottom-quark jet, the number of identified hadronically decaying tau leptons, and the magnitude of the missing transverse energy and of the scalar sum of jet transverse momenta. 

We also place a 95% confidence level upper limit of 1.3% on the branching fraction for the decay of a top quark to a charm quark and a Higgs boson (TOP --&gt; CHARM HIGGS), which translates to a bound on the left- and right-handed top-charm flavor-violating Higgs Yukawa couplings, LAMBDA(HIGGS TOP CHARM) and LAMBDA(HIGGS CHARM TOP) respectively, of SQRT(ABS(LAMBDA(HIGGS TOP CHARM))**2 + ABS(LAMBDA(HIGGS CHARM TOP))**2) &lt; 0.21. 

We also present the product of the acceptance and efficiency for the calculations of the 95% C.L. in several different SUSY scenarios.
DOI: 10.17182/hepdata.64435.v1/t39
title: "Table 39" of "Search for Anomalous Production of Events with Three or More Leptons in $pp$ Collisions at $\sqrt{s} =$ 8 TeV"

description: Observed and expected 95% C.L. limits for the slepton co-NLSP model in the gluino-chargino (wino-like chargino) mass plane are shown.
description: CERN-LHC. A search for physics beyond the standard model in events with at least three leptons is presented. The data sample, corresponding to an integrated luminosity of 19.5 inverse femtobarns of proton-proton collisions with center-of-mass energy sqrt(s) = 8 TeV, was collected by the CMS experiment at the LHC during 2012. The data are divided into exclusive categories based on the number of leptons and their flavor, the presence or absence of an opposite-sign, same-flavor lepton pair (OSSF), the invariant mass of the OSSF pair, the presence or absence of a tagged bottom-quark jet, the number of identified hadronically decaying tau leptons, and the magnitude of the missing transverse energy and of the scalar sum of jet transverse momenta. 

We also place a 95% confidence level upper limit of 1.3% on the branching fraction for the decay of a top quark to a charm quark and a Higgs boson (TOP --&gt; CHARM HIGGS), which translates to a bound on the left- and right-handed top-charm flavor-violating Higgs Yukawa couplings, LAMBDA(HIGGS TOP CHARM) and LAMBDA(HIGGS CHARM TOP) respectively, of SQRT(ABS(LAMBDA(HIGGS TOP CHARM))**2 + ABS(LAMBDA(HIGGS CHARM TOP))**2) &lt; 0.21. 

We also present the product of the acceptance and efficiency for the calculations of the 95% C.L. in several different SUSY scenarios.
DOI: 10.17182/hepdata.64435.v1/t40
title: "Table 40" of "Search for Anomalous Production of Events with Three or More Leptons in $pp$ Collisions at $\sqrt{s} =$ 8 TeV"

description: Observed and expected 95% C.L. limits for the stau-NLSP and stau-NNLSP scenario in the degenerate smuon- and selectron- stau mass plane are shown. Successive instances of SIG(OBS) = SIG(EXP) =0 have been rebinned over M(SELECTRON) to reduce the size of the table.
description: CERN-LHC. A search for physics beyond the standard model in events with at least three leptons is presented. The data sample, corresponding to an integrated luminosity of 19.5 inverse femtobarns of proton-proton collisions with center-of-mass energy sqrt(s) = 8 TeV, was collected by the CMS experiment at the LHC during 2012. The data are divided into exclusive categories based on the number of leptons and their flavor, the presence or absence of an opposite-sign, same-flavor lepton pair (OSSF), the invariant mass of the OSSF pair, the presence or absence of a tagged bottom-quark jet, the number of identified hadronically decaying tau leptons, and the magnitude of the missing transverse energy and of the scalar sum of jet transverse momenta. 

We also place a 95% confidence level upper limit of 1.3% on the branching fraction for the decay of a top quark to a charm quark and a Higgs boson (TOP --&gt; CHARM HIGGS), which translates to a bound on the left- and right-handed top-charm flavor-violating Higgs Yukawa couplings, LAMBDA(HIGGS TOP CHARM) and LAMBDA(HIGGS CHARM TOP) respectively, of SQRT(ABS(LAMBDA(HIGGS TOP CHARM))**2 + ABS(LAMBDA(HIGGS CHARM TOP))**2) &lt; 0.21. 

We also present the product of the acceptance and efficiency for the calculations of the 95% C.L. in several different SUSY scenarios.
DOI: 10.17182/hepdata.64435.v1/t41
title: "Table 41" of "Search for Anomalous Production of Events with Three or More Leptons in $pp$ Collisions at $\sqrt{s} =$ 8 TeV"

description: Observed and expected 95% C.L. limits for the T1tttt model in the gluino-neutralino mass plane are shown.
description: CERN-LHC. A search for physics beyond the standard model in events with at least three leptons is presented. The data sample, corresponding to an integrated luminosity of 19.5 inverse femtobarns of proton-proton collisions with center-of-mass energy sqrt(s) = 8 TeV, was collected by the CMS experiment at the LHC during 2012. The data are divided into exclusive categories based on the number of leptons and their flavor, the presence or absence of an opposite-sign, same-flavor lepton pair (OSSF), the invariant mass of the OSSF pair, the presence or absence of a tagged bottom-quark jet, the number of identified hadronically decaying tau leptons, and the magnitude of the missing transverse energy and of the scalar sum of jet transverse momenta. 

We also place a 95% confidence level upper limit of 1.3% on the branching fraction for the decay of a top quark to a charm quark and a Higgs boson (TOP --&gt; CHARM HIGGS), which translates to a bound on the left- and right-handed top-charm flavor-violating Higgs Yukawa couplings, LAMBDA(HIGGS TOP CHARM) and LAMBDA(HIGGS CHARM TOP) respectively, of SQRT(ABS(LAMBDA(HIGGS TOP CHARM))**2 + ABS(LAMBDA(HIGGS CHARM TOP))**2) &lt; 0.21. 

We also present the product of the acceptance and efficiency for the calculations of the 95% C.L. in several different SUSY scenarios.
DOI: 10.17182/hepdata.64435.v1/t42
title: "Table 42" of "Search for Anomalous Production of Events with Three or More Leptons in $pp$ Collisions at $\sqrt{s} =$ 8 TeV"

description: Observed and expected 95% C.L. limits for the T6ttWW model in the sbottom-chargino mass plane are given.
description: CERN-LHC. A search for physics beyond the standard model in events with at least three leptons is presented. The data sample, corresponding to an integrated luminosity of 19.5 inverse femtobarns of proton-proton collisions with center-of-mass energy sqrt(s) = 8 TeV, was collected by the CMS experiment at the LHC during 2012. The data are divided into exclusive categories based on the number of leptons and their flavor, the presence or absence of an opposite-sign, same-flavor lepton pair (OSSF), the invariant mass of the OSSF pair, the presence or absence of a tagged bottom-quark jet, the number of identified hadronically decaying tau leptons, and the magnitude of the missing transverse energy and of the scalar sum of jet transverse momenta. 

We also place a 95% confidence level upper limit of 1.3% on the branching fraction for the decay of a top quark to a charm quark and a Higgs boson (TOP --&gt; CHARM HIGGS), which translates to a bound on the left- and right-handed top-charm flavor-violating Higgs Yukawa couplings, LAMBDA(HIGGS TOP CHARM) and LAMBDA(HIGGS CHARM TOP) respectively, of SQRT(ABS(LAMBDA(HIGGS TOP CHARM))**2 + ABS(LAMBDA(HIGGS CHARM TOP))**2) &lt; 0.21. 

We also present the product of the acceptance and efficiency for the calculations of the 95% C.L. in several different SUSY scenarios.
DOI: 10.17182/hepdata.64436.v1/t1
title: "Table 1" of "Suppression of $\Upsilon$(1S) at forward rapidity in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: Inclusive Upsilon (1S) Nuclear Modification Factor (Raa) measured in Lead-Lead collisions at sqrt(sNN) = 2.76 TeV in 2.5 &lt; y &lt; 4 and pt &gt; 0 GeV, as a function of the average number of participating nucleons (). Data have been collected in 2011 and the integrated luminosity is ~ 70 inverse microbarn.
description: CERN-LHC. We report on the measurement of the inclusive Upsilon(1S) production in Pb-Pb collisions at sqrt(sNN) = 2.76 TeV carried out at forward rapidity (2.5 &lt; y &lt; 4) and down to zero transverse momentum using its mu+ mu- decay channel with the ALICE detector at the Large Hadron Collider. A strong suppression of the inclusive Upsilon(1S) yield is observed with respect to pp collisions scaled by the number of independent nucleon-nucleon collisions. The nuclear modification factor, for events in the 0-90% centrality range, amounts to 0.30 +- 0.05 (stat) +- 0.04 (syst). The observed Upsilon(1S) suppression increases with the centrality of the collision and is more pronounced than in corresponding mid-rapidity measurements.
DOI: 10.17182/hepdata.64436.v1/t2
title: "Table 2" of "Suppression of $\Upsilon$(1S) at forward rapidity in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

description: Inclusive Upsilon (1S) Nuclear Modification Factor (Raa) measured in Lead-Lead collisions at sqrt(sNN) = 2.76 TeV in 2.5 &lt; y &lt; 4 and pt &gt; 0 GeV, as a function of the rapidity. Data have been collected in 2011 and the integrated luminosity is ~ 70 inverse microbarn.
description: CERN-LHC. We report on the measurement of the inclusive Upsilon(1S) production in Pb-Pb collisions at sqrt(sNN) = 2.76 TeV carried out at forward rapidity (2.5 &lt; y &lt; 4) and down to zero transverse momentum using its mu+ mu- decay channel with the ALICE detector at the Large Hadron Collider. A strong suppression of the inclusive Upsilon(1S) yield is observed with respect to pp collisions scaled by the number of independent nucleon-nucleon collisions. The nuclear modification factor, for events in the 0-90% centrality range, amounts to 0.30 +- 0.05 (stat) +- 0.04 (syst). The observed Upsilon(1S) suppression increases with the centrality of the collision and is more pronounced than in corresponding mid-rapidity measurements.
DOI: 10.17182/hepdata.64481.v1/t1
title: "Table 1" of "Measurement of Feynman-$x$ Spectra of Photons and Neutrons in the Very Forward Direction in Deep-Inelastic Scattering at HERA"

description: The fraction of DIS events with forward photons. For each measurement, the statistical, the uncorrelated systematic uncertainties and the bin-to-bin correlated systematic uncertainties due to the FNC absolute energy scale (EFNC), the measurement of the particle impact position in the FNC (XYFNC) and the model dependence of the data correction (model) are given.
description: DESY-HERA. Measurements of normalised cross sections for the production of photons and neutrons at very small angles with respect to the proton beam direction in deep-inelastic positron-proton scattering at HERA are presented as a function of the Feynman variable, XF, and of the centre-of-mass energy of the virtual photon-proton system, W. The data were taken with the H1 detector in the years 2006 and 2007 and correspond to an integrated luminosity of 131 pb^{-1}. The measurement is restricted to photons and neutrons in the pseudorapidity range ETARAP &gt; 7.9 and covers the range of negative four momentum transfer squared at the positron vertex 6 &lt; Q^2 &lt; 100 GeV^2, of inelasticity 0.05 &lt; Y &lt; 0.6 and of 70 &lt; W &lt; 245 GeV. To test the Feynman scaling hypothesis, the W dependence of the XF dependent cross sections is investigated.
DOI: 10.17182/hepdata.64481.v1/t2
title: "Table 2" of "Measurement of Feynman-$x$ Spectra of Photons and Neutrons in the Very Forward Direction in Deep-Inelastic Scattering at HERA"

description: The fraction of DIS events with forward neutrons. For each measurement, the statistical, the uncorrelated systematic uncertainties and the bin-to-bin correlated systematic uncertainties due to the FNC absolute energy scale (EFNC), the measurement of the particle impact position in the FNC (XYFNC) and the model dependence of the data correction (model) are given.
description: DESY-HERA. Measurements of normalised cross sections for the production of photons and neutrons at very small angles with respect to the proton beam direction in deep-inelastic positron-proton scattering at HERA are presented as a function of the Feynman variable, XF, and of the centre-of-mass energy of the virtual photon-proton system, W. The data were taken with the H1 detector in the years 2006 and 2007 and correspond to an integrated luminosity of 131 pb^{-1}. The measurement is restricted to photons and neutrons in the pseudorapidity range ETARAP &gt; 7.9 and covers the range of negative four momentum transfer squared at the positron vertex 6 &lt; Q^2 &lt; 100 GeV^2, of inelasticity 0.05 &lt; Y &lt; 0.6 and of 70 &lt; W &lt; 245 GeV. To test the Feynman scaling hypothesis, the W dependence of the XF dependent cross sections is investigated.
DOI: 10.17182/hepdata.64481.v1/t3
title: "Table 3" of "Measurement of Feynman-$x$ Spectra of Photons and Neutrons in the Very Forward Direction in Deep-Inelastic Scattering at HERA"

description: Normalised cross sections of forward photon production in DIS as a function of XF. For each measurement, the statistical, the uncorrelated systematic uncertainties and the bin-to-bin correlated systematic uncertainties due to the FNC absolute energy scale (EFNC), the measurement of the particle impact position in the FNC (XYFNC) and the model dependence of the data correction (model) are given.
description: DESY-HERA. Measurements of normalised cross sections for the production of photons and neutrons at very small angles with respect to the proton beam direction in deep-inelastic positron-proton scattering at HERA are presented as a function of the Feynman variable, XF, and of the centre-of-mass energy of the virtual photon-proton system, W. The data were taken with the H1 detector in the years 2006 and 2007 and correspond to an integrated luminosity of 131 pb^{-1}. The measurement is restricted to photons and neutrons in the pseudorapidity range ETARAP &gt; 7.9 and covers the range of negative four momentum transfer squared at the positron vertex 6 &lt; Q^2 &lt; 100 GeV^2, of inelasticity 0.05 &lt; Y &lt; 0.6 and of 70 &lt; W &lt; 245 GeV. To test the Feynman scaling hypothesis, the W dependence of the XF dependent cross sections is investigated.
DOI: 10.17182/hepdata.64481.v1/t4
title: "Table 4" of "Measurement of Feynman-$x$ Spectra of Photons and Neutrons in the Very Forward Direction in Deep-Inelastic Scattering at HERA"

description: Normalised cross sections of forward neutron production in DIS as a function of XF. For each measurement, the statistical, the uncorrelated systematic uncertainties and the bin-to-bin correlated systematic uncertainties due to the FNC absolute energy scale (EFNC), the measurement of the particle impact position in the FNC (XYFNC) and the model dependence of the data correction (model) are given.
description: DESY-HERA. Measurements of normalised cross sections for the production of photons and neutrons at very small angles with respect to the proton beam direction in deep-inelastic positron-proton scattering at HERA are presented as a function of the Feynman variable, XF, and of the centre-of-mass energy of the virtual photon-proton system, W. The data were taken with the H1 detector in the years 2006 and 2007 and correspond to an integrated luminosity of 131 pb^{-1}. The measurement is restricted to photons and neutrons in the pseudorapidity range ETARAP &gt; 7.9 and covers the range of negative four momentum transfer squared at the positron vertex 6 &lt; Q^2 &lt; 100 GeV^2, of inelasticity 0.05 &lt; Y &lt; 0.6 and of 70 &lt; W &lt; 245 GeV. To test the Feynman scaling hypothesis, the W dependence of the XF dependent cross sections is investigated.
DOI: 10.17182/hepdata.64486.v1/t1
title: "Table 1" of "Measurements of the Upsilon(1S), Upsilon(2S), and Upsilon(3S) differential cross sections in pp collisions at sqrt(s) = 7 TeV"

description: The $p_{\rm T}$ bin width, the weighted mean $p_{\rm T}$ within a bin, and the differential cross section times the dimuon branching fraction for the $\Upsilon$(1S), $\Upsilon$(2S), and $\Upsilon$(3S) with $0 &lt; |y| &lt; 0.6$. The statistical and systematic uncertainties in the differential cross section are given as the percentage of the cross section.
description: CERN-LHC. Differential cross sections as a function of transverse momentum $p_\mathrm{T}$ are presented for the production of $\Upsilon(n\mathrm{S})$ ($n$ = 1, 2, 3) states decaying into a pair of muons. Data corresponding to an integrated luminosity of 4.9 fb$^{-1}$ in pp collisions at $\sqrt{s}$ = 7 TeV were collected with the CMS detector at the LHC. The analysis selects events with dimuon absolute rapidity $y$ lower than 1.2 and dimuon transverse momentum in the range of $p_\mathrm{T} $ between 10 and 100 GeV. The measurements show a transition from an exponential to a power-law behavior at $p_\mathrm{T} \approx 20$ GeV for the three $\Upsilon$ states. Above that transition, the $\Upsilon(3\mathrm{S})$ spectrum is significantly harder than that of the $\Upsilon(1\mathrm{S})$ and $\Upsilon(2\mathrm{S})$. The ratios of the $\Upsilon(3\mathrm{S})$ and $\Upsilon(2\mathrm{S})$ differential cross sections to the $\Upsilon(1\mathrm{S})$ cross section show a rise as $p_\mathrm{T}$ increases at low $p_\mathrm{T}$, then become flatter at higher $p_\mathrm{T}$

The tables below list the results of $\Upsilon$(1S), $\Upsilon$(2S) and $\Upsilon$(3S) differential cross sections (SIG) times dimuon branching fraction (B) in three rapidity bins, and ratios thereof. The $\Upsilon$(nS) polarizations measured by CMS are taken as input. The cross sections for different polarization scenarios may be obtained using the corresponding acceptance tables that are also provided below.
DOI: 10.17182/hepdata.64486.v1/t2
title: "Table 2" of "Measurements of the Upsilon(1S), Upsilon(2S), and Upsilon(3S) differential cross sections in pp collisions at sqrt(s) = 7 TeV"

description: The $p_{\rm T}$ bin width, the weighted mean $p_{\rm T}$ within a bin, and the differential cross section times the dimuon branching fraction for the $\Upsilon$(1S), $\Upsilon$(2S), and $\Upsilon$(3S) with $0.6 &lt; |y| &lt; 1.2$. The statistical and systematic uncertainties in the differential cross section are given as the percentage of the cross section.
description: CERN-LHC. Differential cross sections as a function of transverse momentum $p_\mathrm{T}$ are presented for the production of $\Upsilon(n\mathrm{S})$ ($n$ = 1, 2, 3) states decaying into a pair of muons. Data corresponding to an integrated luminosity of 4.9 fb$^{-1}$ in pp collisions at $\sqrt{s}$ = 7 TeV were collected with the CMS detector at the LHC. The analysis selects events with dimuon absolute rapidity $y$ lower than 1.2 and dimuon transverse momentum in the range of $p_\mathrm{T} $ between 10 and 100 GeV. The measurements show a transition from an exponential to a power-law behavior at $p_\mathrm{T} \approx 20$ GeV for the three $\Upsilon$ states. Above that transition, the $\Upsilon(3\mathrm{S})$ spectrum is significantly harder than that of the $\Upsilon(1\mathrm{S})$ and $\Upsilon(2\mathrm{S})$. The ratios of the $\Upsilon(3\mathrm{S})$ and $\Upsilon(2\mathrm{S})$ differential cross sections to the $\Upsilon(1\mathrm{S})$ cross section show a rise as $p_\mathrm{T}$ increases at low $p_\mathrm{T}$, then become flatter at higher $p_\mathrm{T}$

The tables below list the results of $\Upsilon$(1S), $\Upsilon$(2S) and $\Upsilon$(3S) differential cross sections (SIG) times dimuon branching fraction (B) in three rapidity bins, and ratios thereof. The $\Upsilon$(nS) polarizations measured by CMS are taken as input. The cross sections for different polarization scenarios may be obtained using the corresponding acceptance tables that are also provided below.