cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.147283.v1/t157
title: "Efficiency $B^+\to K^+S(\to e^+e^-)$" of "Search for a long-lived spin-0 mediator in $b\to s$ transitions at the Belle II experiment"

description: Efficiencies for $\mathcal{B}($$B^+\to K^+S$$) \times$ $\mathcal{B}($$S\to e^+e^-$)
description: Additional spin-0 particles appear in many extensions of the standard model. We search for long-lived spin-0 particles $S$ in $B$-meson decays mediated by a $b\to s$ quark transition in $e^+e^-$ collisions at the $\Upsilon(4S)$ resonance at the Belle~II experiment. Based on a sample corresponding to an integrated luminosity of 189$\,\text{fb}^{-1}$, we observe no evidence for signal. We set model-independent upper limits on the product of branching fractions $\mathcal{B}(B^0\to K^*(892)^0(\to K^+\pi^-)S)\times \mathcal{B}(S\to x^+x^-)$ and $\mathcal{B}(B^+\to K^+S)\times \mathcal{B}(S\to x^+x^-)$, where $x^+x^-$ indicates $e^+e^-, \mu^+\mu^-, \pi^+\pi^-$, or $K^+K^-$, as functions of $S$ mass and lifetime at the level of $10^{-7}$.
DOI: 10.17182/hepdata.147283.v1/t158
title: "Efficiency $B^+\to K^+S(\to \mu^+\mu^-)$" of "Search for a long-lived spin-0 mediator in $b\to s$ transitions at the Belle II experiment"

description: Efficiencies for $\mathcal{B}($$B^+\to K^+S$$) \times$ $\mathcal{B}($$S\to \mu^+\mu^-$)
description: Additional spin-0 particles appear in many extensions of the standard model. We search for long-lived spin-0 particles $S$ in $B$-meson decays mediated by a $b\to s$ quark transition in $e^+e^-$ collisions at the $\Upsilon(4S)$ resonance at the Belle~II experiment. Based on a sample corresponding to an integrated luminosity of 189$\,\text{fb}^{-1}$, we observe no evidence for signal. We set model-independent upper limits on the product of branching fractions $\mathcal{B}(B^0\to K^*(892)^0(\to K^+\pi^-)S)\times \mathcal{B}(S\to x^+x^-)$ and $\mathcal{B}(B^+\to K^+S)\times \mathcal{B}(S\to x^+x^-)$, where $x^+x^-$ indicates $e^+e^-, \mu^+\mu^-, \pi^+\pi^-$, or $K^+K^-$, as functions of $S$ mass and lifetime at the level of $10^{-7}$.
DOI: 10.17182/hepdata.147283.v1/t159
title: "Efficiency $B^+\to K^+S(\to \pi^+\pi^-)$" of "Search for a long-lived spin-0 mediator in $b\to s$ transitions at the Belle II experiment"

description: Efficiencies for $\mathcal{B}($$B^+\to K^+S$$) \times$ $\mathcal{B}($$S\to \pi^+\pi^-$)
description: Additional spin-0 particles appear in many extensions of the standard model. We search for long-lived spin-0 particles $S$ in $B$-meson decays mediated by a $b\to s$ quark transition in $e^+e^-$ collisions at the $\Upsilon(4S)$ resonance at the Belle~II experiment. Based on a sample corresponding to an integrated luminosity of 189$\,\text{fb}^{-1}$, we observe no evidence for signal. We set model-independent upper limits on the product of branching fractions $\mathcal{B}(B^0\to K^*(892)^0(\to K^+\pi^-)S)\times \mathcal{B}(S\to x^+x^-)$ and $\mathcal{B}(B^+\to K^+S)\times \mathcal{B}(S\to x^+x^-)$, where $x^+x^-$ indicates $e^+e^-, \mu^+\mu^-, \pi^+\pi^-$, or $K^+K^-$, as functions of $S$ mass and lifetime at the level of $10^{-7}$.
DOI: 10.17182/hepdata.147283.v1/t160
title: "Efficiency $B^+\to K^+S(\to K^+K^-)$" of "Search for a long-lived spin-0 mediator in $b\to s$ transitions at the Belle II experiment"

description: Efficiencies for $\mathcal{B}($$B^+\to K^+S$$) \times$ $\mathcal{B}($$S\to K^+K^-$)
description: Additional spin-0 particles appear in many extensions of the standard model. We search for long-lived spin-0 particles $S$ in $B$-meson decays mediated by a $b\to s$ quark transition in $e^+e^-$ collisions at the $\Upsilon(4S)$ resonance at the Belle~II experiment. Based on a sample corresponding to an integrated luminosity of 189$\,\text{fb}^{-1}$, we observe no evidence for signal. We set model-independent upper limits on the product of branching fractions $\mathcal{B}(B^0\to K^*(892)^0(\to K^+\pi^-)S)\times \mathcal{B}(S\to x^+x^-)$ and $\mathcal{B}(B^+\to K^+S)\times \mathcal{B}(S\to x^+x^-)$, where $x^+x^-$ indicates $e^+e^-, \mu^+\mu^-, \pi^+\pi^-$, or $K^+K^-$, as functions of $S$ mass and lifetime at the level of $10^{-7}$.
DOI: 10.17182/hepdata.147283.v1/t161
title: "Efficiency $B^0\to K^{*0}S(\to e^+e^-)$" of "Search for a long-lived spin-0 mediator in $b\to s$ transitions at the Belle II experiment"

description: Efficiencies for $\mathcal{B}($$B^0\to K^{*0}(\to K^+\pi^-)S$$) \times$ $\mathcal{B}($$S\to e^+e^-$)
description: Additional spin-0 particles appear in many extensions of the standard model. We search for long-lived spin-0 particles $S$ in $B$-meson decays mediated by a $b\to s$ quark transition in $e^+e^-$ collisions at the $\Upsilon(4S)$ resonance at the Belle~II experiment. Based on a sample corresponding to an integrated luminosity of 189$\,\text{fb}^{-1}$, we observe no evidence for signal. We set model-independent upper limits on the product of branching fractions $\mathcal{B}(B^0\to K^*(892)^0(\to K^+\pi^-)S)\times \mathcal{B}(S\to x^+x^-)$ and $\mathcal{B}(B^+\to K^+S)\times \mathcal{B}(S\to x^+x^-)$, where $x^+x^-$ indicates $e^+e^-, \mu^+\mu^-, \pi^+\pi^-$, or $K^+K^-$, as functions of $S$ mass and lifetime at the level of $10^{-7}$.
DOI: 10.17182/hepdata.147283.v1/t162
title: "Efficiency $B^0\to K^{*0}S(\to \mu^+\mu^-)$" of "Search for a long-lived spin-0 mediator in $b\to s$ transitions at the Belle II experiment"

description: Efficiencies for $\mathcal{B}($$B^0\to K^{*0}(\to K^+\pi^-)S$$) \times$ $\mathcal{B}($$S\to \mu^+\mu^-$)
description: Additional spin-0 particles appear in many extensions of the standard model. We search for long-lived spin-0 particles $S$ in $B$-meson decays mediated by a $b\to s$ quark transition in $e^+e^-$ collisions at the $\Upsilon(4S)$ resonance at the Belle~II experiment. Based on a sample corresponding to an integrated luminosity of 189$\,\text{fb}^{-1}$, we observe no evidence for signal. We set model-independent upper limits on the product of branching fractions $\mathcal{B}(B^0\to K^*(892)^0(\to K^+\pi^-)S)\times \mathcal{B}(S\to x^+x^-)$ and $\mathcal{B}(B^+\to K^+S)\times \mathcal{B}(S\to x^+x^-)$, where $x^+x^-$ indicates $e^+e^-, \mu^+\mu^-, \pi^+\pi^-$, or $K^+K^-$, as functions of $S$ mass and lifetime at the level of $10^{-7}$.
DOI: 10.17182/hepdata.147283.v1/t163
title: "Efficiency $B^0\to K^{*0}S(\to \pi^+\pi^-)$" of "Search for a long-lived spin-0 mediator in $b\to s$ transitions at the Belle II experiment"

description: Efficiencies for $\mathcal{B}($$B^0\to K^{*0}(\to K^+\pi^-)S$$) \times$ $\mathcal{B}($$S\to \pi^+\pi^-$)
description: Additional spin-0 particles appear in many extensions of the standard model. We search for long-lived spin-0 particles $S$ in $B$-meson decays mediated by a $b\to s$ quark transition in $e^+e^-$ collisions at the $\Upsilon(4S)$ resonance at the Belle~II experiment. Based on a sample corresponding to an integrated luminosity of 189$\,\text{fb}^{-1}$, we observe no evidence for signal. We set model-independent upper limits on the product of branching fractions $\mathcal{B}(B^0\to K^*(892)^0(\to K^+\pi^-)S)\times \mathcal{B}(S\to x^+x^-)$ and $\mathcal{B}(B^+\to K^+S)\times \mathcal{B}(S\to x^+x^-)$, where $x^+x^-$ indicates $e^+e^-, \mu^+\mu^-, \pi^+\pi^-$, or $K^+K^-$, as functions of $S$ mass and lifetime at the level of $10^{-7}$.
DOI: 10.17182/hepdata.147283.v1/t164
title: "Efficiency $B^0\to K^{*0}S(\to K^+K^-)$" of "Search for a long-lived spin-0 mediator in $b\to s$ transitions at the Belle II experiment"

description: Efficiencies for $\mathcal{B}($$B^0\to K^{*0}(\to K^+\pi^-)S$$) \times$ $\mathcal{B}($$S\to K^+K^-$)
description: Additional spin-0 particles appear in many extensions of the standard model. We search for long-lived spin-0 particles $S$ in $B$-meson decays mediated by a $b\to s$ quark transition in $e^+e^-$ collisions at the $\Upsilon(4S)$ resonance at the Belle~II experiment. Based on a sample corresponding to an integrated luminosity of 189$\,\text{fb}^{-1}$, we observe no evidence for signal. We set model-independent upper limits on the product of branching fractions $\mathcal{B}(B^0\to K^*(892)^0(\to K^+\pi^-)S)\times \mathcal{B}(S\to x^+x^-)$ and $\mathcal{B}(B^+\to K^+S)\times \mathcal{B}(S\to x^+x^-)$, where $x^+x^-$ indicates $e^+e^-, \mu^+\mu^-, \pi^+\pi^-$, or $K^+K^-$, as functions of $S$ mass and lifetime at the level of $10^{-7}$.
DOI: 10.17182/hepdata.147308.v1/t1
title: "Limits - Majorana, (re, ru, rt) = (0.0, 1.0, 0.0)" of "Search for long-lived heavy neutrinos in the decays of B mesons produced in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% CL upper limits on $|V_\mathrm{N}|^2$ as a function of $m_\mathrm{N}$ for the mixing scenario ($r_e$, $r_\mu$, $r_\tau$) = (0.0, 1.0, 0.0) and in the Majorana scenario.
description: No data abstract available.
DOI: 10.17182/hepdata.147308.v1/t2
title: "Limits - Majorana, (re, ru, rt) = (0.0, 0.5, 0.5)" of "Search for long-lived heavy neutrinos in the decays of B mesons produced in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% CL upper limits on $|V_\mathrm{N}|^2$ as a function of $m_\mathrm{N}$ for the mixing scenario ($r_e$, $r_\mu$, $r_\tau$) = (0.0, 0.5, 0.5) and in the Majorana scenario.
description: No data abstract available.
DOI: 10.17182/hepdata.147308.v1/t3
title: "Limits - Majorana, (re, ru, rt) = (0.5, 0.5, 0.0)" of "Search for long-lived heavy neutrinos in the decays of B mesons produced in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% CL upper limits on $|V_\mathrm{N}|^2$ as a function of $m_\mathrm{N}$ for the mixing scenario ($r_e$, $r_\mu$, $r_\tau$) = (0.5, 0.5, 0.0) and in the Majorana scenario.
description: No data abstract available.
DOI: 10.17182/hepdata.147308.v1/t4
title: "Limits - Majorana, (re, ru, rt) = (0.33, 0.33, 0.33)" of "Search for long-lived heavy neutrinos in the decays of B mesons produced in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% CL upper limits on $|V_\mathrm{N}|^2$ as a function of $m_\mathrm{N}$ for the mixing scenario ($r_e$, $r_\mu$, $r_\tau$) = (0.33, 0.33, 0.33) and in the Majorana scenario.
description: No data abstract available.
DOI: 10.17182/hepdata.147308.v1/t5
title: "Limits - Dirac-like, (re, ru, rt) = (0.0, 1.0, 0.0)" of "Search for long-lived heavy neutrinos in the decays of B mesons produced in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% CL upper limits on $|V_\mathrm{N}|^2$ as a function of $m_\mathrm{N}$ for the mixing scenario ($r_e$, $r_\mu$, $r_\tau$) = (0.0, 1.0, 0.0) and in the Dirac-like scenario.
description: No data abstract available.
DOI: 10.17182/hepdata.147308.v1/t6
title: "Limits - Dirac-like, (re, ru, rt) = (0.0, 0.5, 0.5)" of "Search for long-lived heavy neutrinos in the decays of B mesons produced in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% CL upper limits on $|V_\mathrm{N}|^2$ as a function of $m_\mathrm{N}$ for the mixing scenario ($r_e$, $r_\mu$, $r_\tau$) = (0.0, 0.5, 0.5) and in the Dirac-like scenario.
description: No data abstract available.
DOI: 10.17182/hepdata.147308.v1/t7
title: "Limits - Dirac-like, (re, ru, rt) = (0.5, 0.5, 0.0)" of "Search for long-lived heavy neutrinos in the decays of B mesons produced in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% CL upper limits on $|V_\mathrm{N}|^2$ as a function of $m_\mathrm{N}$ for the mixing scenario ($r_e$, $r_\mu$, $r_\tau$) = (0.5, 0.5, 0.0) and in the Dirac-like scenario.
description: No data abstract available.
DOI: 10.17182/hepdata.147308.v1/t8
title: "Limits - Dirac-like, (re, ru, rt) = (0.33, 0.33, 0.33)" of "Search for long-lived heavy neutrinos in the decays of B mesons produced in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% CL upper limits on $|V_\mathrm{N}|^2$ as a function of $m_\mathrm{N}$ for the mixing scenario ($r_e$, $r_\mu$, $r_\tau$) = (0.33, 0.33, 0.33) and in the Dirac-like scenario.
description: No data abstract available.
DOI: 10.17182/hepdata.147308.v1/t9
title: "Ternary Plot - 1.0 GeV, Majorana" of "Search for long-lived heavy neutrinos in the decays of B mesons produced in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed 95% CL lower limits on $c\tau_\mathrm{N}$ as functions of the mixing ratios ($r_e$, $r_\mu$, $r_\tau$) for a fixed N mass of 1.0 GeV in the Majorana scenario.
description: No data abstract available.
DOI: 10.48610/9f79469
title: Australian Writing and Rock Music

description: This dataset is part of the AUSTLIT database. It collects writing by Australian rock musicians and/or about Australian rock music within AUSTLIT's scope.
DOI: 10.17182/hepdata.147308.v1/t10
title: "Ternary Plot - 1.5 GeV, Majorana" of "Search for long-lived heavy neutrinos in the decays of B mesons produced in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed 95% CL lower limits on $c\tau_\mathrm{N}$ as functions of the mixing ratios ($r_e$, $r_\mu$, $r_\tau$) for a fixed N mass of 1.5 GeV in the Majorana scenario.
description: No data abstract available.
DOI: 10.17182/hepdata.147308.v1/t11
title: "Ternary Plot - 2.0 GeV, Majorana" of "Search for long-lived heavy neutrinos in the decays of B mesons produced in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed 95% CL lower limits on $c\tau_\mathrm{N}$ as functions of the mixing ratios ($r_e$, $r_\mu$, $r_\tau$) for a fixed N mass of 2.0 GeV in the Majorana scenario.
description: No data abstract available.
DOI: 10.17182/hepdata.147308.v1/t12
title: "Ternary Plot - 1.0 GeV, Dirac-like" of "Search for long-lived heavy neutrinos in the decays of B mesons produced in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed 95% CL lower limits on $c\tau_\mathrm{N}$ as functions of the mixing ratios ($r_e$, $r_\mu$, $r_\tau$) for a fixed N mass of 1.0 GeV in the Dirac-like scenario.
description: No data abstract available.
DOI: 10.17182/hepdata.147308.v1/t13
title: "Ternary Plot - 1.5 GeV, Dirac-like" of "Search for long-lived heavy neutrinos in the decays of B mesons produced in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed 95% CL lower limits on $c\tau_\mathrm{N}$ as functions of the mixing ratios ($r_e$, $r_\mu$, $r_\tau$) for a fixed N mass of 1.5 GeV in the Dirac-like scenario.
description: No data abstract available.
DOI: 10.17182/hepdata.147308.v1/t14
title: "Ternary Plot - 2.0 GeV, Dirac-like" of "Search for long-lived heavy neutrinos in the decays of B mesons produced in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed 95% CL lower limits on $c\tau_\mathrm{N}$ as functions of the mixing ratios ($r_e$, $r_\mu$, $r_\tau$) for a fixed N mass of 2.0 GeV in the Dirac-like scenario.
description: No data abstract available.
DOI: 10.17182/hepdata.147309.v1/t1
title: "Figure 1" of "Search for the decay of the Higgs boson to a pair of light pseudoscalar bosons in the final state with four bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Post-fit BDT distributions in the WH channel extracted with the ma = 60 GeV signal hypothesis. Signal regions for the 3b (upper) and 4b (lower) event categories are shown separately for the electron (left) and muon (right) channels. The dotted lines WH20 GeV, WH60 GeV, illustrate the shapes of the signal template normalised to the SM cross section times a branching fraction B(H → aa → bbbb) = 1 and scaled by the factors indicated in the figure. The horizontal error bars indicate the bin width.
description: A search is presented for the decay of the 125 GeV Higgs boson (H) to a pair of new light pseudoscalar bosons (a), followed by the prompt decay of each a boson to a bottom quark-antiquark pair, $\textrm{H} \rightarrow$ aa $\rightarrow$ bbbb. The analysis is performed using a data sample of proton-proton collisions collected with the CMS detector at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 $\textrm{fb}^{-1}$. To reduce the background from standard model processes, the search requires the Higgs boson to be produced in association with a leptonically decaying W or Z boson. The analysis probes the production of new light bosons in a $15 &lt; \textrm{m}_{a} &lt; 60$ GeV mass range. Assuming the standard model predictions for the Higgs boson production cross sections for pp $\rightarrow$ WH and ZH, model independent upper limits at 95% confidence level are derived for the branching fraction $\mathcal{B}(\textrm{H} \rightarrow$ aa $\rightarrow$ bbbb). The combined WH and ZH observed upper limit on the branching fraction ranges from 1.10 for $\textrm{m}_{a} = 20$ GeV to 0.36 for $\textrm{m}_{a} = 60$ GeV, complementing other measurements in the $\mu\mu\tau\tau$, $\tau\tau\tau\tau$ and bb$\ell\ell$ ($\ell=\mu, \tau$) channels.
DOI: 10.17182/hepdata.147309.v1/t2
title: "Figure 2" of "Search for the decay of the Higgs boson to a pair of light pseudoscalar bosons in the final state with four bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Post-fit BDT distributions in the ZH channel extracted with the ma = 60 GeV signal hypothesis. Signal regions for the 3b (upper) and 4b (lower) event categories are shown separately for the electron (left) and muon (right) channels. The dotted lines ZH20 GeV and ZH60 GeV, illustrate the shapes of the signal template normalised to the SM cross section times a branching fraction B(H → aa → bbbb) = 1 and scaled by the factors indicated in the figure. The horizontal error bars indicate the bin width.
description: A search is presented for the decay of the 125 GeV Higgs boson (H) to a pair of new light pseudoscalar bosons (a), followed by the prompt decay of each a boson to a bottom quark-antiquark pair, $\textrm{H} \rightarrow$ aa $\rightarrow$ bbbb. The analysis is performed using a data sample of proton-proton collisions collected with the CMS detector at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 $\textrm{fb}^{-1}$. To reduce the background from standard model processes, the search requires the Higgs boson to be produced in association with a leptonically decaying W or Z boson. The analysis probes the production of new light bosons in a $15 &lt; \textrm{m}_{a} &lt; 60$ GeV mass range. Assuming the standard model predictions for the Higgs boson production cross sections for pp $\rightarrow$ WH and ZH, model independent upper limits at 95% confidence level are derived for the branching fraction $\mathcal{B}(\textrm{H} \rightarrow$ aa $\rightarrow$ bbbb). The combined WH and ZH observed upper limit on the branching fraction ranges from 1.10 for $\textrm{m}_{a} = 20$ GeV to 0.36 for $\textrm{m}_{a} = 60$ GeV, complementing other measurements in the $\mu\mu\tau\tau$, $\tau\tau\tau\tau$ and bb$\ell\ell$ ($\ell=\mu, \tau$) channels.
DOI: 10.17182/hepdata.147309.v1/t3
title: "Figure 3" of "Search for the decay of the Higgs boson to a pair of light pseudoscalar bosons in the final state with four bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Model independent 95% CL upper limits on σ(VH) B(H → aa → bbbb)/σ(SM) for the WH channel (upper), the ZH channel (middle), and the combination of both channels (lower), where “a” is a new pseudoscalar particle decaying through a → bb, and σ(SM) is the SM Higgs boson production cross section.
description: A search is presented for the decay of the 125 GeV Higgs boson (H) to a pair of new light pseudoscalar bosons (a), followed by the prompt decay of each a boson to a bottom quark-antiquark pair, $\textrm{H} \rightarrow$ aa $\rightarrow$ bbbb. The analysis is performed using a data sample of proton-proton collisions collected with the CMS detector at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 $\textrm{fb}^{-1}$. To reduce the background from standard model processes, the search requires the Higgs boson to be produced in association with a leptonically decaying W or Z boson. The analysis probes the production of new light bosons in a $15 &lt; \textrm{m}_{a} &lt; 60$ GeV mass range. Assuming the standard model predictions for the Higgs boson production cross sections for pp $\rightarrow$ WH and ZH, model independent upper limits at 95% confidence level are derived for the branching fraction $\mathcal{B}(\textrm{H} \rightarrow$ aa $\rightarrow$ bbbb). The combined WH and ZH observed upper limit on the branching fraction ranges from 1.10 for $\textrm{m}_{a} = 20$ GeV to 0.36 for $\textrm{m}_{a} = 60$ GeV, complementing other measurements in the $\mu\mu\tau\tau$, $\tau\tau\tau\tau$ and bb$\ell\ell$ ($\ell=\mu, \tau$) channels.
DOI: 10.17182/hepdata.147309.v1/t4
title: "Table 3" of "Search for the decay of the Higgs boson to a pair of light pseudoscalar bosons in the final state with four bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Example description
description: A search is presented for the decay of the 125 GeV Higgs boson (H) to a pair of new light pseudoscalar bosons (a), followed by the prompt decay of each a boson to a bottom quark-antiquark pair, $\textrm{H} \rightarrow$ aa $\rightarrow$ bbbb. The analysis is performed using a data sample of proton-proton collisions collected with the CMS detector at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 $\textrm{fb}^{-1}$. To reduce the background from standard model processes, the search requires the Higgs boson to be produced in association with a leptonically decaying W or Z boson. The analysis probes the production of new light bosons in a $15 &lt; \textrm{m}_{a} &lt; 60$ GeV mass range. Assuming the standard model predictions for the Higgs boson production cross sections for pp $\rightarrow$ WH and ZH, model independent upper limits at 95% confidence level are derived for the branching fraction $\mathcal{B}(\textrm{H} \rightarrow$ aa $\rightarrow$ bbbb). The combined WH and ZH observed upper limit on the branching fraction ranges from 1.10 for $\textrm{m}_{a} = 20$ GeV to 0.36 for $\textrm{m}_{a} = 60$ GeV, complementing other measurements in the $\mu\mu\tau\tau$, $\tau\tau\tau\tau$ and bb$\ell\ell$ ($\ell=\mu, \tau$) channels.
DOI: 10.17182/hepdata.147309.v1/t5
title: "Table 1" of "Search for the decay of the Higgs boson to a pair of light pseudoscalar bosons in the final state with four bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Example description
description: A search is presented for the decay of the 125 GeV Higgs boson (H) to a pair of new light pseudoscalar bosons (a), followed by the prompt decay of each a boson to a bottom quark-antiquark pair, $\textrm{H} \rightarrow$ aa $\rightarrow$ bbbb. The analysis is performed using a data sample of proton-proton collisions collected with the CMS detector at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 $\textrm{fb}^{-1}$. To reduce the background from standard model processes, the search requires the Higgs boson to be produced in association with a leptonically decaying W or Z boson. The analysis probes the production of new light bosons in a $15 &lt; \textrm{m}_{a} &lt; 60$ GeV mass range. Assuming the standard model predictions for the Higgs boson production cross sections for pp $\rightarrow$ WH and ZH, model independent upper limits at 95% confidence level are derived for the branching fraction $\mathcal{B}(\textrm{H} \rightarrow$ aa $\rightarrow$ bbbb). The combined WH and ZH observed upper limit on the branching fraction ranges from 1.10 for $\textrm{m}_{a} = 20$ GeV to 0.36 for $\textrm{m}_{a} = 60$ GeV, complementing other measurements in the $\mu\mu\tau\tau$, $\tau\tau\tau\tau$ and bb$\ell\ell$ ($\ell=\mu, \tau$) channels.