cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.82127.v1/t11
title: "Table11" of "Search for a singly produced vector-like quark B decaying to a b quark and a Higgs boson in a fully hadronic final state using boosted topologies"

description: The median observed and expected 95% CL upper limits on the product of the B quark production cross section and branching fraction as a function of the signal mass, for the resonance width/mass equal to 20% scenario. The results are shown for the combination of 0 and &gt;0 forward-jet categories.
description: A search is presented for single production of heavy vector-like quarks (B) that decay to a Higgs boson and a b quark, with the Higgs boson decaying to a highly boosted bb pair reconstructed as a single collimated jet. The analysis is based on data collected by the CMS experiment in proton-proton collisions at √s = 13 TeV, corresponding to an integrated luminosity of 35.9fb−1. The data are consistent with background ex- pectations, and upper limits at 95% confidence level on the product of the B quark cross section and the branching fraction are obtained in the range 1.28–0.07 pb, for a narrow B quark with a mass between 700 and 1800 GeV. The production of B quarks with widths of 10, 20 and 30% of the resonance mass is also considered, and the sen- sitivities obtained are similar to those achieved in the narrow width case. This is the first search at the CERN LHC for the single production of a B quark through its fully hadronic decay channel, and the first study considering finite resonance widths of the B quark.
DOI: 10.17182/hepdata.82127.v1/t12
title: "Table12" of "Search for a singly produced vector-like quark B decaying to a b quark and a Higgs boson in a fully hadronic final state using boosted topologies"

description: The median observed and expected 95% CL upper limits on the product of the B quark production cross section and branching fraction as a function of the signal mass, for the resonance width/mass equal to 30% scenario. The results are shown for the combination of 0 and &gt;0 forward-jet categories.
description: A search is presented for single production of heavy vector-like quarks (B) that decay to a Higgs boson and a b quark, with the Higgs boson decaying to a highly boosted bb pair reconstructed as a single collimated jet. The analysis is based on data collected by the CMS experiment in proton-proton collisions at √s = 13 TeV, corresponding to an integrated luminosity of 35.9fb−1. The data are consistent with background ex- pectations, and upper limits at 95% confidence level on the product of the B quark cross section and the branching fraction are obtained in the range 1.28–0.07 pb, for a narrow B quark with a mass between 700 and 1800 GeV. The production of B quarks with widths of 10, 20 and 30% of the resonance mass is also considered, and the sen- sitivities obtained are similar to those achieved in the narrow width case. This is the first search at the CERN LHC for the single production of a B quark through its fully hadronic decay channel, and the first study considering finite resonance widths of the B quark.
DOI: 10.17182/hepdata.82127.v1/t13
title: "Table13" of "Search for a singly produced vector-like quark B decaying to a b quark and a Higgs boson in a fully hadronic final state using boosted topologies"

description: Observed and expected fitted number of events in the signal ranges of 800 &lt; mB &lt; 1500, and expected signal at mB = 1000 GeV. The multijet background is obtained from data, while the yields for the other sources of background are obtained from MC simulation. The combined statistical and systematic uncertainties correspond to the quadrature of the statistical and systematic uncertainties.
description: A search is presented for single production of heavy vector-like quarks (B) that decay to a Higgs boson and a b quark, with the Higgs boson decaying to a highly boosted bb pair reconstructed as a single collimated jet. The analysis is based on data collected by the CMS experiment in proton-proton collisions at √s = 13 TeV, corresponding to an integrated luminosity of 35.9fb−1. The data are consistent with background ex- pectations, and upper limits at 95% confidence level on the product of the B quark cross section and the branching fraction are obtained in the range 1.28–0.07 pb, for a narrow B quark with a mass between 700 and 1800 GeV. The production of B quarks with widths of 10, 20 and 30% of the resonance mass is also considered, and the sen- sitivities obtained are similar to those achieved in the narrow width case. This is the first search at the CERN LHC for the single production of a B quark through its fully hadronic decay channel, and the first study considering finite resonance widths of the B quark.
DOI: 10.17182/hepdata.82127.v1/t14
title: "Table14" of "Search for a singly produced vector-like quark B decaying to a b quark and a Higgs boson in a fully hadronic final state using boosted topologies"

description: Observed and expected fitted number of events in the signal ranges 1500 &lt; mB &lt; 1800 , and expected signal at mB = 1800 GeV. The multijet background is obtained from data, while the yields for the other sources of background are obtained from MC simulation. The combined statistical and systematic uncertainties correspond to the quadrature of the statistical and systematic uncertainties.
description: A search is presented for single production of heavy vector-like quarks (B) that decay to a Higgs boson and a b quark, with the Higgs boson decaying to a highly boosted bb pair reconstructed as a single collimated jet. The analysis is based on data collected by the CMS experiment in proton-proton collisions at √s = 13 TeV, corresponding to an integrated luminosity of 35.9fb−1. The data are consistent with background ex- pectations, and upper limits at 95% confidence level on the product of the B quark cross section and the branching fraction are obtained in the range 1.28–0.07 pb, for a narrow B quark with a mass between 700 and 1800 GeV. The production of B quarks with widths of 10, 20 and 30% of the resonance mass is also considered, and the sen- sitivities obtained are similar to those achieved in the narrow width case. This is the first search at the CERN LHC for the single production of a B quark through its fully hadronic decay channel, and the first study considering finite resonance widths of the B quark.
DOI: 10.17182/hepdata.82210.v1/t1
title: "Table 1" of "Measurement of $\Upsilon$ production in $pp$ collisions at $\sqrt{s}$= 13 TeV"

description: Double-differential cross-sections times dimuon branching fraction in different bins of $p_T$ and $y$ for $\Upsilon$(1S) (in pb). The first uncertainty is statistical and the second is systematic.
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=13$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 277 pb$^{-1}$. The production cross-sections 
 and ratios of cross-sections are measured as functions
of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$
and $2.0
DOI: 10.17182/hepdata.82210.v1/t2
title: "Table 2" of "Measurement of $\Upsilon$ production in $pp$ collisions at $\sqrt{s}$= 13 TeV"

description: Double-differential cross-sections times dimuon branching fraction in different bins of $p_T$ and $y$ for $\Upsilon$(2S) (in pb). The first uncertainty is statistical and the second is systematic.
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=13$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 277 pb$^{-1}$. The production cross-sections 
 and ratios of cross-sections are measured as functions
of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$
and $2.0
DOI: 10.17182/hepdata.82210.v1/t3
title: "Table 3" of "Measurement of $\Upsilon$ production in $pp$ collisions at $\sqrt{s}$= 13 TeV"

description: Double-differential cross-sections times dimuon branching fraction in different bins of $p_T$ and $y$ for $\Upsilon$(3S) (in pb). The first uncertainty is statistical and the second is systematic.
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=13$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 277 pb$^{-1}$. The production cross-sections 
 and ratios of cross-sections are measured as functions
of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$
and $2.0
DOI: 10.17182/hepdata.82210.v1/t4
title: "Table 4" of "Measurement of $\Upsilon$ production in $pp$ collisions at $\sqrt{s}$= 13 TeV"

description: Differential cross-sections multiplied by dimuon branching fractions for $\Upsilon$(1S), $\Upsilon$(2S) and $\Upsilon$(3S) states versus $p_T$ integrated over $y$ between 2.0 and 4.5.
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=13$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 277 pb$^{-1}$. The production cross-sections 
 and ratios of cross-sections are measured as functions
of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$
and $2.0
DOI: 10.17182/hepdata.82210.v1/t5
title: "Table 5" of "Measurement of $\Upsilon$ production in $pp$ collisions at $\sqrt{s}$= 13 TeV"

description: Differential cross-sections multiplied by dimuon branching fractions for $\Upsilon$(1S), $\Upsilon$(2S) and $\Upsilon$(3S) states versus $y$ integrated over $p_T$ from 0 to 15 GeV/c.
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=13$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 277 pb$^{-1}$. The production cross-sections 
 and ratios of cross-sections are measured as functions
of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$
and $2.0
DOI: 10.17182/hepdata.82210.v1/t6
title: "Table 6" of "Measurement of $\Upsilon$ production in $pp$ collisions at $\sqrt{s}$= 13 TeV"

description: Ratios of double-differential cross-sections times dimuon branching fractions for $\Upsilon$(2S) to $\Upsilon$(1S).
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=13$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 277 pb$^{-1}$. The production cross-sections 
 and ratios of cross-sections are measured as functions
of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$
and $2.0
DOI: 10.17182/hepdata.82210.v1/t7
title: "Table 7" of "Measurement of $\Upsilon$ production in $pp$ collisions at $\sqrt{s}$= 13 TeV"

description: Ratios of double-differential cross-sections times dimuon branching fractions for $\Upsilon$(3S) to $\Upsilon$(1S).
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=13$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 277 pb$^{-1}$. The production cross-sections 
 and ratios of cross-sections are measured as functions
of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$
and $2.0
DOI: 10.17182/hepdata.82210.v1/t8
title: "Table 8" of "Measurement of $\Upsilon$ production in $pp$ collisions at $\sqrt{s}$= 13 TeV"

description: Ratios of differential cross-sections times dimuon branching fractions versus $p_T$ over $y$ for $\Upsilon$(2S) to $\Upsilon$(1S) and $\Upsilon$(3S) to $\Upsilon$(1S).
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=13$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 277 pb$^{-1}$. The production cross-sections 
 and ratios of cross-sections are measured as functions
of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$
and $2.0
DOI: 10.17182/hepdata.82210.v1/t9
title: "Table 9" of "Measurement of $\Upsilon$ production in $pp$ collisions at $\sqrt{s}$= 13 TeV"

description: Ratios of differential cross-sections times dimuon branching fractions versus $y$ over $p_T$ for $\Upsilon$(2S) to $\Upsilon$(1S) and $\Upsilon$(3S) to $\Upsilon$(1S).
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=13$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 277 pb$^{-1}$. The production cross-sections 
 and ratios of cross-sections are measured as functions
of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$
and $2.0
DOI: 10.17182/hepdata.82210.v1/t10
title: "Table 10" of "Measurement of $\Upsilon$ production in $pp$ collisions at $\sqrt{s}$= 13 TeV"

description: The cross-section ratios between 13 TeV and 8 TeV in different bins of $p_T$ and $y$ for $\Upsilon$(1S).
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=13$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 277 pb$^{-1}$. The production cross-sections 
 and ratios of cross-sections are measured as functions
of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$
and $2.0
DOI: 10.17182/hepdata.82210.v1/t11
title: "Table 11" of "Measurement of $\Upsilon$ production in $pp$ collisions at $\sqrt{s}$= 13 TeV"

description: The cross-section ratios between 13 TeV and 8 TeV in different bins of $p_T$ and $y$ for $\Upsilon$(2S).
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=13$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 277 pb$^{-1}$. The production cross-sections 
 and ratios of cross-sections are measured as functions
of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$
and $2.0
DOI: 10.17182/hepdata.82210.v1/t12
title: "Table 12" of "Measurement of $\Upsilon$ production in $pp$ collisions at $\sqrt{s}$= 13 TeV"

description: The cross-section ratios between 13 TeV and 8 TeV in different bins of $p_T$ and $y$ for $\Upsilon$(3S).
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=13$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 277 pb$^{-1}$. The production cross-sections 
 and ratios of cross-sections are measured as functions
of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$
and $2.0
DOI: 10.17182/hepdata.82210.v1/t13
title: "Table 13" of "Measurement of $\Upsilon$ production in $pp$ collisions at $\sqrt{s}$= 13 TeV"

description: Ratios of differential cross-sections between 13 TeV and 8 TeV measurements versus $p_T$ over $y$ for $\Upsilon$(1S), $\Upsilon$(2S) and $\Upsilon$(3S).
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=13$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 277 pb$^{-1}$. The production cross-sections 
 and ratios of cross-sections are measured as functions
of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$
and $2.0
DOI: 10.17182/hepdata.82210.v1/t14
title: "Table 14" of "Measurement of $\Upsilon$ production in $pp$ collisions at $\sqrt{s}$= 13 TeV"

description: Ratios of differential cross-sections between 13 TeV and 8 TeV measurements versus $y$ over $p_T$ for $\Upsilon$(1S), $\Upsilon$(2S) and $\Upsilon$(3S).
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=13$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 277 pb$^{-1}$. The production cross-sections 
 and ratios of cross-sections are measured as functions
of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$
and $2.0
DOI: 10.17182/hepdata.82211.v1/t1
title: "Table 1" of "First Measurement of the Muon Anti-Neutrino Double-Differential Charged Current Quasi-Elastic Cross Section"

description: Flux (neutrinos /cm^2/Protons on Target/50 MeV).
description: The largest sample ever recorded of $\bar{\nu}_\mu$ charged-current quasielastic (CCQE, $\bar{\nu}_\mu p \to \mu^{+} n$) candidate events is used to produce the minimally model-dependent, flux-integrated double-differential cross section $\frac{d^{2}\sigma}{dT_\mu d\textrm{cos}\, \theta_\mu}$ for $\bar{\nu}_\mu$ CCQE for a mineral oil target. This measurement exploits the large statistics of the MiniBooNE antineutrino-mode sample and provides the most complete information of this process to date. In order to facilitate historical comparisons, the flux-unfolded total cross section and single-differential cross section on both mineral oil and on carbon are also reported. Numbers are taken from the MiniBooNE Data Release (http://www-boone.fnal.gov/for_physicists/data_release/ccqe_nubar/).
DOI: 10.17182/hepdata.82211.v1/t2
title: "Table 2" of "First Measurement of the Muon Anti-Neutrino Double-Differential Charged Current Quasi-Elastic Cross Section"

description: The MiniBooNE $\bar{\nu}_\mu$ CCQE double-differential cross section on mineral oil, together with the shape uncertainty, in units of fb/GeV $(10^{-39}~\mbox{cm}^2/\mbox{GeV})$. Data is given in 0.1 GeV bins of $T_\mu$ (columns) and 0.1 bins of $\,\textrm{cos}\, \theta_\mu$ (rows). Not included in the table is the total normalization uncertainty of 13.0$\%$.
description: The largest sample ever recorded of $\bar{\nu}_\mu$ charged-current quasielastic (CCQE, $\bar{\nu}_\mu p \to \mu^{+} n$) candidate events is used to produce the minimally model-dependent, flux-integrated double-differential cross section $\frac{d^{2}\sigma}{dT_\mu d\textrm{cos}\, \theta_\mu}$ for $\bar{\nu}_\mu$ CCQE for a mineral oil target. This measurement exploits the large statistics of the MiniBooNE antineutrino-mode sample and provides the most complete information of this process to date. In order to facilitate historical comparisons, the flux-unfolded total cross section and single-differential cross section on both mineral oil and on carbon are also reported. Numbers are taken from the MiniBooNE Data Release (http://www-boone.fnal.gov/for_physicists/data_release/ccqe_nubar/).
DOI: 10.17182/hepdata.82211.v1/t3
title: "Table 3" of "First Measurement of the Muon Anti-Neutrino Double-Differential Charged Current Quasi-Elastic Cross Section"

description: CCQE-like background in units of fb/GeV $(10^{-39}~\mbox{cm}^2)/\mbox{GeV}$ to the MiniBooNE $\bar{\nu}_\mu$ CCQE double-differential cross section on mineral oil. In this configuration, the hydrogen scattering component is treated as signal and is not included in the CCQE-like background.
description: The largest sample ever recorded of $\bar{\nu}_\mu$ charged-current quasielastic (CCQE, $\bar{\nu}_\mu p \to \mu^{+} n$) candidate events is used to produce the minimally model-dependent, flux-integrated double-differential cross section $\frac{d^{2}\sigma}{dT_\mu d\textrm{cos}\, \theta_\mu}$ for $\bar{\nu}_\mu$ CCQE for a mineral oil target. This measurement exploits the large statistics of the MiniBooNE antineutrino-mode sample and provides the most complete information of this process to date. In order to facilitate historical comparisons, the flux-unfolded total cross section and single-differential cross section on both mineral oil and on carbon are also reported. Numbers are taken from the MiniBooNE Data Release (http://www-boone.fnal.gov/for_physicists/data_release/ccqe_nubar/).
DOI: 10.17182/hepdata.82211.v1/t4
title: "Table 4" of "First Measurement of the Muon Anti-Neutrino Double-Differential Charged Current Quasi-Elastic Cross Section"

description: The predicted CC1$\pi^{-}$ background in units of fb/GeV $(10^{-39}~\mbox{cm}^2)/\mbox{GeV}$ . This background corresponds to an empirical adjustment of the Rein-Sehgal calculation based on the MiniBooNE CC1$\pi^{+}$ data.
description: The largest sample ever recorded of $\bar{\nu}_\mu$ charged-current quasielastic (CCQE, $\bar{\nu}_\mu p \to \mu^{+} n$) candidate events is used to produce the minimally model-dependent, flux-integrated double-differential cross section $\frac{d^{2}\sigma}{dT_\mu d\textrm{cos}\, \theta_\mu}$ for $\bar{\nu}_\mu$ CCQE for a mineral oil target. This measurement exploits the large statistics of the MiniBooNE antineutrino-mode sample and provides the most complete information of this process to date. In order to facilitate historical comparisons, the flux-unfolded total cross section and single-differential cross section on both mineral oil and on carbon are also reported. Numbers are taken from the MiniBooNE Data Release (http://www-boone.fnal.gov/for_physicists/data_release/ccqe_nubar/).
DOI: 10.17182/hepdata.82211.v1/t5
title: "Table 5" of "First Measurement of the Muon Anti-Neutrino Double-Differential Charged Current Quasi-Elastic Cross Section"

description: The MiniBooNE numub single differential cross section $\frac{d\sigma}{dQ^2_{QE}}$ on mineral oil, shape error, and the predicted CCQE-like and CC1$\pi^{-}$ backgrounds in units of fb $(10^{-39} \mbox{cm}^2)$. Not included in the table is the total normalization error of 13.0$\%$.
description: The largest sample ever recorded of $\bar{\nu}_\mu$ charged-current quasielastic (CCQE, $\bar{\nu}_\mu p \to \mu^{+} n$) candidate events is used to produce the minimally model-dependent, flux-integrated double-differential cross section $\frac{d^{2}\sigma}{dT_\mu d\textrm{cos}\, \theta_\mu}$ for $\bar{\nu}_\mu$ CCQE for a mineral oil target. This measurement exploits the large statistics of the MiniBooNE antineutrino-mode sample and provides the most complete information of this process to date. In order to facilitate historical comparisons, the flux-unfolded total cross section and single-differential cross section on both mineral oil and on carbon are also reported. Numbers are taken from the MiniBooNE Data Release (http://www-boone.fnal.gov/for_physicists/data_release/ccqe_nubar/).
DOI: 10.17182/hepdata.82211.v1/t6
title: "Table 6" of "First Measurement of the Muon Anti-Neutrino Double-Differential Charged Current Quasi-Elastic Cross Section"

description: The MiniBooNE $\bar{\nu}_\mu$ CCQE total cross section on mineral oil, total and shape errors, and predicted CCQE-like and CC1$\pi^{-}$ backgrounds in bins of $E_\nu^{\textrm{QE,RFG}}$ and units of fb $(10^{-39} \mbox{cm}^2)$. The total error includes both the shape and normalization uncertainties. Note that the total error is incorrectly quoted as a power of 10 too low in the paper and the preprint. It is corrected in the resource file from which these data here are taken.
description: The largest sample ever recorded of $\bar{\nu}_\mu$ charged-current quasielastic (CCQE, $\bar{\nu}_\mu p \to \mu^{+} n$) candidate events is used to produce the minimally model-dependent, flux-integrated double-differential cross section $\frac{d^{2}\sigma}{dT_\mu d\textrm{cos}\, \theta_\mu}$ for $\bar{\nu}_\mu$ CCQE for a mineral oil target. This measurement exploits the large statistics of the MiniBooNE antineutrino-mode sample and provides the most complete information of this process to date. In order to facilitate historical comparisons, the flux-unfolded total cross section and single-differential cross section on both mineral oil and on carbon are also reported. Numbers are taken from the MiniBooNE Data Release (http://www-boone.fnal.gov/for_physicists/data_release/ccqe_nubar/).