cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.89936.v1/t2
title: "Figure 2a ($H\rightarrow\gamma\gamma$)" of "Measurement and interpretation of differential cross sections for Higgs boson production at $\sqrt{s}=$ 13 TeV"

description: Higgs boson transverse momentum spectrum, $H\rightarrow\gamma\gamma$
description: Differential Higgs boson ($H$) production cross sections are sensitive probes for physics beyond the standard model. New physics may contribute in the gluon-gluon fusion loop, the dominant Higgs boson production mechanism at the LHC, and manifest itself through deviations from the distributions predicted by the standard model. Combined spectra for the $H\to\gamma\gamma$, $H\to ZZ$, and $H\to b \overline{b}$ decay channels and the inclusive Higgs boson production cross section are presented, based on proton-proton collision data recorded with the CMS detector at $\sqrt{s}=13$\TeV corresponding to an integrated luminosity of 35.9 fb${}^{-1}$. The transverse momentum spectrum is used to place limits on the Higgs boson couplings to the top, bottom, and charm quarks, as well as its direct coupling to the gluon field. No significant deviations from the standard model are observed in any differential distribution. The measured total cross section is $61.1\pm 6.0 \text{(stat)} \pm 3.7 \text{(syst)}$ pb, and the precision of the measurement of the differential cross section of the Higgs boson transverse momentum is improved by about 15% with respect to the $H\to\gamma\gamma$ channel alone.
DOI: 10.17182/hepdata.89936.v1/t3
title: "Figure 2a ($H\rightarrow ZZ$)" of "Measurement and interpretation of differential cross sections for Higgs boson production at $\sqrt{s}=$ 13 TeV"

description: Higgs boson transverse momentum spectrum, $H\rightarrow ZZ$
description: Differential Higgs boson ($H$) production cross sections are sensitive probes for physics beyond the standard model. New physics may contribute in the gluon-gluon fusion loop, the dominant Higgs boson production mechanism at the LHC, and manifest itself through deviations from the distributions predicted by the standard model. Combined spectra for the $H\to\gamma\gamma$, $H\to ZZ$, and $H\to b \overline{b}$ decay channels and the inclusive Higgs boson production cross section are presented, based on proton-proton collision data recorded with the CMS detector at $\sqrt{s}=13$\TeV corresponding to an integrated luminosity of 35.9 fb${}^{-1}$. The transverse momentum spectrum is used to place limits on the Higgs boson couplings to the top, bottom, and charm quarks, as well as its direct coupling to the gluon field. No significant deviations from the standard model are observed in any differential distribution. The measured total cross section is $61.1\pm 6.0 \text{(stat)} \pm 3.7 \text{(syst)}$ pb, and the precision of the measurement of the differential cross section of the Higgs boson transverse momentum is improved by about 15% with respect to the $H\to\gamma\gamma$ channel alone.
DOI: 10.17182/hepdata.89936.v1/t4
title: "Figure 2a ($H\rightarrow b\overline{b}$)" of "Measurement and interpretation of differential cross sections for Higgs boson production at $\sqrt{s}=$ 13 TeV"

description: Higgs boson transverse momentum spectrum, $H\rightarrow b\overline{b}$
description: Differential Higgs boson ($H$) production cross sections are sensitive probes for physics beyond the standard model. New physics may contribute in the gluon-gluon fusion loop, the dominant Higgs boson production mechanism at the LHC, and manifest itself through deviations from the distributions predicted by the standard model. Combined spectra for the $H\to\gamma\gamma$, $H\to ZZ$, and $H\to b \overline{b}$ decay channels and the inclusive Higgs boson production cross section are presented, based on proton-proton collision data recorded with the CMS detector at $\sqrt{s}=13$\TeV corresponding to an integrated luminosity of 35.9 fb${}^{-1}$. The transverse momentum spectrum is used to place limits on the Higgs boson couplings to the top, bottom, and charm quarks, as well as its direct coupling to the gluon field. No significant deviations from the standard model are observed in any differential distribution. The measured total cross section is $61.1\pm 6.0 \text{(stat)} \pm 3.7 \text{(syst)}$ pb, and the precision of the measurement of the differential cross section of the Higgs boson transverse momentum is improved by about 15% with respect to the $H\to\gamma\gamma$ channel alone.
DOI: 10.17182/hepdata.89936.v1/t5
title: "Figure 2b (Combination)" of "Measurement and interpretation of differential cross sections for Higgs boson production at $\sqrt{s}=$ 13 TeV"

description: Combined Higgs boson transverse momentum spectrum, ggH only
description: Differential Higgs boson ($H$) production cross sections are sensitive probes for physics beyond the standard model. New physics may contribute in the gluon-gluon fusion loop, the dominant Higgs boson production mechanism at the LHC, and manifest itself through deviations from the distributions predicted by the standard model. Combined spectra for the $H\to\gamma\gamma$, $H\to ZZ$, and $H\to b \overline{b}$ decay channels and the inclusive Higgs boson production cross section are presented, based on proton-proton collision data recorded with the CMS detector at $\sqrt{s}=13$\TeV corresponding to an integrated luminosity of 35.9 fb${}^{-1}$. The transverse momentum spectrum is used to place limits on the Higgs boson couplings to the top, bottom, and charm quarks, as well as its direct coupling to the gluon field. No significant deviations from the standard model are observed in any differential distribution. The measured total cross section is $61.1\pm 6.0 \text{(stat)} \pm 3.7 \text{(syst)}$ pb, and the precision of the measurement of the differential cross section of the Higgs boson transverse momentum is improved by about 15% with respect to the $H\to\gamma\gamma$ channel alone.
DOI: 10.17182/hepdata.89936.v1/t6
title: "Figure 3 (Combination)" of "Measurement and interpretation of differential cross sections for Higgs boson production at $\sqrt{s}=$ 13 TeV"

description: Combined Higgs boson jet multiplicity spectrum
description: Differential Higgs boson ($H$) production cross sections are sensitive probes for physics beyond the standard model. New physics may contribute in the gluon-gluon fusion loop, the dominant Higgs boson production mechanism at the LHC, and manifest itself through deviations from the distributions predicted by the standard model. Combined spectra for the $H\to\gamma\gamma$, $H\to ZZ$, and $H\to b \overline{b}$ decay channels and the inclusive Higgs boson production cross section are presented, based on proton-proton collision data recorded with the CMS detector at $\sqrt{s}=13$\TeV corresponding to an integrated luminosity of 35.9 fb${}^{-1}$. The transverse momentum spectrum is used to place limits on the Higgs boson couplings to the top, bottom, and charm quarks, as well as its direct coupling to the gluon field. No significant deviations from the standard model are observed in any differential distribution. The measured total cross section is $61.1\pm 6.0 \text{(stat)} \pm 3.7 \text{(syst)}$ pb, and the precision of the measurement of the differential cross section of the Higgs boson transverse momentum is improved by about 15% with respect to the $H\to\gamma\gamma$ channel alone.
DOI: 10.17182/hepdata.89936.v1/t7
title: "Figure 3 ($H\rightarrow\gamma\gamma$)" of "Measurement and interpretation of differential cross sections for Higgs boson production at $\sqrt{s}=$ 13 TeV"

description: Higgs boson jet multiplicity spectrum, $H\rightarrow\gamma\gamma$
description: Differential Higgs boson ($H$) production cross sections are sensitive probes for physics beyond the standard model. New physics may contribute in the gluon-gluon fusion loop, the dominant Higgs boson production mechanism at the LHC, and manifest itself through deviations from the distributions predicted by the standard model. Combined spectra for the $H\to\gamma\gamma$, $H\to ZZ$, and $H\to b \overline{b}$ decay channels and the inclusive Higgs boson production cross section are presented, based on proton-proton collision data recorded with the CMS detector at $\sqrt{s}=13$\TeV corresponding to an integrated luminosity of 35.9 fb${}^{-1}$. The transverse momentum spectrum is used to place limits on the Higgs boson couplings to the top, bottom, and charm quarks, as well as its direct coupling to the gluon field. No significant deviations from the standard model are observed in any differential distribution. The measured total cross section is $61.1\pm 6.0 \text{(stat)} \pm 3.7 \text{(syst)}$ pb, and the precision of the measurement of the differential cross section of the Higgs boson transverse momentum is improved by about 15% with respect to the $H\to\gamma\gamma$ channel alone.
DOI: 10.17182/hepdata.89936.v1/t8
title: "Figure 3 ($H\rightarrow ZZ$)" of "Measurement and interpretation of differential cross sections for Higgs boson production at $\sqrt{s}=$ 13 TeV"

description: Higgs boson jet multiplicity spectrum, $H\rightarrow ZZ$
description: Differential Higgs boson ($H$) production cross sections are sensitive probes for physics beyond the standard model. New physics may contribute in the gluon-gluon fusion loop, the dominant Higgs boson production mechanism at the LHC, and manifest itself through deviations from the distributions predicted by the standard model. Combined spectra for the $H\to\gamma\gamma$, $H\to ZZ$, and $H\to b \overline{b}$ decay channels and the inclusive Higgs boson production cross section are presented, based on proton-proton collision data recorded with the CMS detector at $\sqrt{s}=13$\TeV corresponding to an integrated luminosity of 35.9 fb${}^{-1}$. The transverse momentum spectrum is used to place limits on the Higgs boson couplings to the top, bottom, and charm quarks, as well as its direct coupling to the gluon field. No significant deviations from the standard model are observed in any differential distribution. The measured total cross section is $61.1\pm 6.0 \text{(stat)} \pm 3.7 \text{(syst)}$ pb, and the precision of the measurement of the differential cross section of the Higgs boson transverse momentum is improved by about 15% with respect to the $H\to\gamma\gamma$ channel alone.
DOI: 10.17182/hepdata.89936.v1/t10
title: "Figure 4 ($H\rightarrow\gamma\gamma$)" of "Measurement and interpretation of differential cross sections for Higgs boson production at $\sqrt{s}=$ 13 TeV"

description: Higgs boson rapidity spectrum, $H\rightarrow\gamma\gamma$
description: Differential Higgs boson ($H$) production cross sections are sensitive probes for physics beyond the standard model. New physics may contribute in the gluon-gluon fusion loop, the dominant Higgs boson production mechanism at the LHC, and manifest itself through deviations from the distributions predicted by the standard model. Combined spectra for the $H\to\gamma\gamma$, $H\to ZZ$, and $H\to b \overline{b}$ decay channels and the inclusive Higgs boson production cross section are presented, based on proton-proton collision data recorded with the CMS detector at $\sqrt{s}=13$\TeV corresponding to an integrated luminosity of 35.9 fb${}^{-1}$. The transverse momentum spectrum is used to place limits on the Higgs boson couplings to the top, bottom, and charm quarks, as well as its direct coupling to the gluon field. No significant deviations from the standard model are observed in any differential distribution. The measured total cross section is $61.1\pm 6.0 \text{(stat)} \pm 3.7 \text{(syst)}$ pb, and the precision of the measurement of the differential cross section of the Higgs boson transverse momentum is improved by about 15% with respect to the $H\to\gamma\gamma$ channel alone.
DOI: 10.17182/hepdata.89936.v1/t11
title: "Figure 4 ($H\rightarrow ZZ$)" of "Measurement and interpretation of differential cross sections for Higgs boson production at $\sqrt{s}=$ 13 TeV"

description: Higgs boson rapidity spectrum, $H\rightarrow ZZ$
description: Differential Higgs boson ($H$) production cross sections are sensitive probes for physics beyond the standard model. New physics may contribute in the gluon-gluon fusion loop, the dominant Higgs boson production mechanism at the LHC, and manifest itself through deviations from the distributions predicted by the standard model. Combined spectra for the $H\to\gamma\gamma$, $H\to ZZ$, and $H\to b \overline{b}$ decay channels and the inclusive Higgs boson production cross section are presented, based on proton-proton collision data recorded with the CMS detector at $\sqrt{s}=13$\TeV corresponding to an integrated luminosity of 35.9 fb${}^{-1}$. The transverse momentum spectrum is used to place limits on the Higgs boson couplings to the top, bottom, and charm quarks, as well as its direct coupling to the gluon field. No significant deviations from the standard model are observed in any differential distribution. The measured total cross section is $61.1\pm 6.0 \text{(stat)} \pm 3.7 \text{(syst)}$ pb, and the precision of the measurement of the differential cross section of the Higgs boson transverse momentum is improved by about 15% with respect to the $H\to\gamma\gamma$ channel alone.
DOI: 10.17182/hepdata.89936.v1/t12
title: "Figure 5 (Combination)" of "Measurement and interpretation of differential cross sections for Higgs boson production at $\sqrt{s}=$ 13 TeV"

description: Combined leading jet transverse momentum spectrum
description: Differential Higgs boson ($H$) production cross sections are sensitive probes for physics beyond the standard model. New physics may contribute in the gluon-gluon fusion loop, the dominant Higgs boson production mechanism at the LHC, and manifest itself through deviations from the distributions predicted by the standard model. Combined spectra for the $H\to\gamma\gamma$, $H\to ZZ$, and $H\to b \overline{b}$ decay channels and the inclusive Higgs boson production cross section are presented, based on proton-proton collision data recorded with the CMS detector at $\sqrt{s}=13$\TeV corresponding to an integrated luminosity of 35.9 fb${}^{-1}$. The transverse momentum spectrum is used to place limits on the Higgs boson couplings to the top, bottom, and charm quarks, as well as its direct coupling to the gluon field. No significant deviations from the standard model are observed in any differential distribution. The measured total cross section is $61.1\pm 6.0 \text{(stat)} \pm 3.7 \text{(syst)}$ pb, and the precision of the measurement of the differential cross section of the Higgs boson transverse momentum is improved by about 15% with respect to the $H\to\gamma\gamma$ channel alone.
DOI: 10.17182/hepdata.89936.v1/t13
title: "Figure 5 ($H\rightarrow\gamma\gamma$)" of "Measurement and interpretation of differential cross sections for Higgs boson production at $\sqrt{s}=$ 13 TeV"

description: Leading jet transverse momentum spectrum, $H\rightarrow\gamma\gamma$
description: Differential Higgs boson ($H$) production cross sections are sensitive probes for physics beyond the standard model. New physics may contribute in the gluon-gluon fusion loop, the dominant Higgs boson production mechanism at the LHC, and manifest itself through deviations from the distributions predicted by the standard model. Combined spectra for the $H\to\gamma\gamma$, $H\to ZZ$, and $H\to b \overline{b}$ decay channels and the inclusive Higgs boson production cross section are presented, based on proton-proton collision data recorded with the CMS detector at $\sqrt{s}=13$\TeV corresponding to an integrated luminosity of 35.9 fb${}^{-1}$. The transverse momentum spectrum is used to place limits on the Higgs boson couplings to the top, bottom, and charm quarks, as well as its direct coupling to the gluon field. No significant deviations from the standard model are observed in any differential distribution. The measured total cross section is $61.1\pm 6.0 \text{(stat)} \pm 3.7 \text{(syst)}$ pb, and the precision of the measurement of the differential cross section of the Higgs boson transverse momentum is improved by about 15% with respect to the $H\to\gamma\gamma$ channel alone.
DOI: 10.17182/hepdata.89936.v1/t14
title: "Figure 5 ($H\rightarrow ZZ$)" of "Measurement and interpretation of differential cross sections for Higgs boson production at $\sqrt{s}=$ 13 TeV"

description: Leading jet transverse momentum spectrum, $H\rightarrow ZZ$
description: Differential Higgs boson ($H$) production cross sections are sensitive probes for physics beyond the standard model. New physics may contribute in the gluon-gluon fusion loop, the dominant Higgs boson production mechanism at the LHC, and manifest itself through deviations from the distributions predicted by the standard model. Combined spectra for the $H\to\gamma\gamma$, $H\to ZZ$, and $H\to b \overline{b}$ decay channels and the inclusive Higgs boson production cross section are presented, based on proton-proton collision data recorded with the CMS detector at $\sqrt{s}=13$\TeV corresponding to an integrated luminosity of 35.9 fb${}^{-1}$. The transverse momentum spectrum is used to place limits on the Higgs boson couplings to the top, bottom, and charm quarks, as well as its direct coupling to the gluon field. No significant deviations from the standard model are observed in any differential distribution. The measured total cross section is $61.1\pm 6.0 \text{(stat)} \pm 3.7 \text{(syst)}$ pb, and the precision of the measurement of the differential cross section of the Higgs boson transverse momentum is improved by about 15% with respect to the $H\to\gamma\gamma$ channel alone.
DOI: 10.17182/hepdata.89936.v1/t9
title: "Figure 4 (Combination)" of "Measurement and interpretation of differential cross sections for Higgs boson production at $\sqrt{s}=$ 13 TeV"

description: Combined Higgs boson rapidity spectrum
description: Differential Higgs boson ($H$) production cross sections are sensitive probes for physics beyond the standard model. New physics may contribute in the gluon-gluon fusion loop, the dominant Higgs boson production mechanism at the LHC, and manifest itself through deviations from the distributions predicted by the standard model. Combined spectra for the $H\to\gamma\gamma$, $H\to ZZ$, and $H\to b \overline{b}$ decay channels and the inclusive Higgs boson production cross section are presented, based on proton-proton collision data recorded with the CMS detector at $\sqrt{s}=13$\TeV corresponding to an integrated luminosity of 35.9 fb${}^{-1}$. The transverse momentum spectrum is used to place limits on the Higgs boson couplings to the top, bottom, and charm quarks, as well as its direct coupling to the gluon field. No significant deviations from the standard model are observed in any differential distribution. The measured total cross section is $61.1\pm 6.0 \text{(stat)} \pm 3.7 \text{(syst)}$ pb, and the precision of the measurement of the differential cross section of the Higgs boson transverse momentum is improved by about 15% with respect to the $H\to\gamma\gamma$ channel alone.
DOI: 10.17182/hepdata.89937.v2/t1
title: "Figure 5-a" of "Search for heavy Higgs bosons decaying to a top quark pair in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: Model-independent constraints on the coupling strength modifier as a function of the heavy scalar boson mass, for a relative width of 0.5%.
description: A search is presented for additional scalar (H) or pseudoscalar (A) Higgs bosons decaying to a top quark pair in proton-proton collisions at a center-of-mass energy of 13 TeV. The data set analyzed corresponds to an integrated luminosity of 35.9 fb-1 collected by the CMS experiment at the LHC. Final states with one or two charged leptons are considered. The invariant mass of the reconstructed top quark pair system and variables that are sensitive to the spin of the particles decaying into the top quark pair are used to search for signatures of the H or A bosons. The interference with the standard model top quark pair background is taken into account. A moderate signal-like deviation compatible with an A boson with a mass of 400 GeV is observed with a global significance of 1.9 standard deviations. New stringent constraints are reported on the strength of the coupling of the hypothetical bosons to the top quark, with the mass of the bosons ranging from 400 to 750 GeV and their total relative width from 0.5 to 25%. The results of the search are also interpreted in a minimal supersymmetric standard model scenario. Values of m_A from 400 to 700 GeV are probed, and a region with values of tan(beta) below 1.0 to 1.5, depending on m_A, is excluded at 95% confidence level.
DOI: 10.17182/hepdata.89937.v2/t2
title: "Figure 5-b" of "Search for heavy Higgs bosons decaying to a top quark pair in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: Model-independent constraints on the coupling strength modifier as a function of the heavy scalar boson mass, for a relative width of 1.0%.
description: A search is presented for additional scalar (H) or pseudoscalar (A) Higgs bosons decaying to a top quark pair in proton-proton collisions at a center-of-mass energy of 13 TeV. The data set analyzed corresponds to an integrated luminosity of 35.9 fb-1 collected by the CMS experiment at the LHC. Final states with one or two charged leptons are considered. The invariant mass of the reconstructed top quark pair system and variables that are sensitive to the spin of the particles decaying into the top quark pair are used to search for signatures of the H or A bosons. The interference with the standard model top quark pair background is taken into account. A moderate signal-like deviation compatible with an A boson with a mass of 400 GeV is observed with a global significance of 1.9 standard deviations. New stringent constraints are reported on the strength of the coupling of the hypothetical bosons to the top quark, with the mass of the bosons ranging from 400 to 750 GeV and their total relative width from 0.5 to 25%. The results of the search are also interpreted in a minimal supersymmetric standard model scenario. Values of m_A from 400 to 700 GeV are probed, and a region with values of tan(beta) below 1.0 to 1.5, depending on m_A, is excluded at 95% confidence level.
DOI: 10.17182/hepdata.89937.v2/t3
title: "Figure 5-c" of "Search for heavy Higgs bosons decaying to a top quark pair in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: Model-independent constraints on the coupling strength modifier as a function of the heavy scalar boson mass, for a relative width of 2.5%.
description: A search is presented for additional scalar (H) or pseudoscalar (A) Higgs bosons decaying to a top quark pair in proton-proton collisions at a center-of-mass energy of 13 TeV. The data set analyzed corresponds to an integrated luminosity of 35.9 fb-1 collected by the CMS experiment at the LHC. Final states with one or two charged leptons are considered. The invariant mass of the reconstructed top quark pair system and variables that are sensitive to the spin of the particles decaying into the top quark pair are used to search for signatures of the H or A bosons. The interference with the standard model top quark pair background is taken into account. A moderate signal-like deviation compatible with an A boson with a mass of 400 GeV is observed with a global significance of 1.9 standard deviations. New stringent constraints are reported on the strength of the coupling of the hypothetical bosons to the top quark, with the mass of the bosons ranging from 400 to 750 GeV and their total relative width from 0.5 to 25%. The results of the search are also interpreted in a minimal supersymmetric standard model scenario. Values of m_A from 400 to 700 GeV are probed, and a region with values of tan(beta) below 1.0 to 1.5, depending on m_A, is excluded at 95% confidence level.