cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.82715.v1/t4
title: "Table 4" of "Measurement of $D_s^{\pm}$ production asymmetry in $pp$ collisions at $\sqrt{s} =7$ and 8 TeV"

description: The covariance matrix for the kinematic bins matrix of the $D_s^+$ production asymmetry measured using the combined $\sqrt{s} =7$ and 8 TeV data sets (corresponding to Table 1). The statistical and systematic uncertainties are combined. The kinematic bins are indexed as follows: the three rapidity bins, y, in the range from 2.0 to 4.5 are indexed with $i_y$ ranging from 0 to 2 with the following bin edges: 2.0, 3.0, 3.5, 4.5. The four $p_{\rm T}$ bins in the range from 2.5 to 25.0 GeV/c are indexed with $i_{p_T}$ from 0 to 3 with the following bin edges: 2.5, 4.7, 6.5, 8.5, 25.0 GeV/c. The index of a kinematic bins is then given by: $i_{\rm bin} = 4 \times i_y + i_{p_T}$.
description: The inclusive $D_s^{\pm}$ production asymmetry is measured in $pp$ collisions collected by the LHCb experiment at centre-of-mass energies of $\sqrt{s} =7$ and 8 TeV. Promptly produced $D_s^{\pm}$ mesons are used, which decay as $D_s^{\pm}\to\phi\pi^{\pm}$, with $\phi\to K^+K^-$. The measurement is performed in bins of transverse momentum, $p_{\rm T}$, and rapidity, $y$, covering the range $2.5
DOI: 10.17182/hepdata.82715.v1/t5
title: "Table 5" of "Measurement of $D_s^{\pm}$ production asymmetry in $pp$ collisions at $\sqrt{s} =7$ and 8 TeV"

description: The covariance matrix for the kinematic bins matrix of the $D_s^+$ production asymmetry measured using the $\sqrt{s} =7$ TeV data set (corresponding to Table 2). The statistical and systematic uncertainties are combined. The kinematic bins are indexed as follows: the three rapidity bins, y, in the range from 2.0 to 4.5 are indexed with $i_y$ ranging from 0 to 2 with the following bin edges: 2.0, 3.0, 3.5, 4.5. The four $p_{\rm T}$ bins in the range from 2.5 to 25.0 GeV/c are indexed with $i_{p_T}$ from 0 to 3 with the following bin edges: 2.5, 4.7, 6.5, 8.5, 25.0 GeV/c. The index of a kinematic bins is then given by: $i_{\rm bin} = 4 \times i_y + i_{p_T}$.
description: The inclusive $D_s^{\pm}$ production asymmetry is measured in $pp$ collisions collected by the LHCb experiment at centre-of-mass energies of $\sqrt{s} =7$ and 8 TeV. Promptly produced $D_s^{\pm}$ mesons are used, which decay as $D_s^{\pm}\to\phi\pi^{\pm}$, with $\phi\to K^+K^-$. The measurement is performed in bins of transverse momentum, $p_{\rm T}$, and rapidity, $y$, covering the range $2.5
DOI: 10.17182/hepdata.82715.v1/t6
title: "Table 6" of "Measurement of $D_s^{\pm}$ production asymmetry in $pp$ collisions at $\sqrt{s} =7$ and 8 TeV"

description: The covariance matrix for the kinematic bins matrix of the $D_s^+$ production asymmetry measured using the $\sqrt{s} =8$ TeV data set (corresponding to Table 3). The statistical and systematic uncertainties are combined. The kinematic bins are indexed as follows: the three rapidity bins, y, in the range from 2.0 to 4.5 are indexed with $i_y$ ranging from 0 to 2 with the following bin edges: 2.0, 3.0, 3.5, 4.5. The four $p_{\rm T}$ bins in the range from 2.5 to 25.0 GeV/c are indexed with $i_{p_T}$ from 0 to 3 with the following bin edges: 2.5, 4.7, 6.5, 8.5, 25.0 GeV/c. The index of a kinematic bins is then given by: $i_{\rm bin} = 4 \times i_y + i_{p_T}$.
description: The inclusive $D_s^{\pm}$ production asymmetry is measured in $pp$ collisions collected by the LHCb experiment at centre-of-mass energies of $\sqrt{s} =7$ and 8 TeV. Promptly produced $D_s^{\pm}$ mesons are used, which decay as $D_s^{\pm}\to\phi\pi^{\pm}$, with $\phi\to K^+K^-$. The measurement is performed in bins of transverse momentum, $p_{\rm T}$, and rapidity, $y$, covering the range $2.5
DOI: 10.17182/hepdata.82818.v1/t1
title: "Table 1" of "Search for Higgs boson pair production in the $\gamma\gamma b\bar{b}$ final state with 13 TeV $pp$ collision data collected by the ATLAS experiment"

description: Number of expected and observed events in the 1- and 2-tag categories in the resonant analysis. The loose and tight selections are not orthogonal.
description: CERN-LHC, ATLAS.
Limits on pair production of Higgs bosons in the final state where one Higgs boson decays to two photons and the other to a b-quark together with its antiparticle.
The search is based on 36.1 +/- 1.2 fb^{-1} of pp collisions at sqrt{s} = 13 TeV recorded in 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider.
Data include at least one b-tagged jet and two well-identified isolated photons.
The search is sensitive to both resonant and non-resonant production of Higgs boson pairs.
Preselection:
- 2 jets with pT &gt; 25 GeV and |eta| &lt; 2.5, not within DeltaR = 0.4 of an isolated photon candidate or DeltaR = 0.2 of an isolated electron candidate
- Among isolated photons take the two with highest pT and require ET &gt; 0.35 * m_gammagamma and ET &gt; 0.25 * m_gammagamma respectively
- 105 &lt; m_gammagamma &lt; 160 GeV
After this preselection, two further kinematic selections are defined.
Loose selection:
- jet1 pT &gt; 40 GeV, jet2 pT &gt; 25 GeV
- 80 &lt; m_jj &lt; 140 GeV
- |m_gammagamma - m_H| &lt; 4.7 GeV (resonant search only)
Tight selection:
- jet1 pT &gt; 100 GeV, jet2 pT &gt; 30 GeV
- 90 &lt; m_jj &lt; 140 GeV
- |m_gammagamma - m_H| &lt; 4.3 GeV (resonant search only)
For each of these selections, a 1-tag and 2-tag category are considered.
2-tag category:
- both jets pass a 70% efficient b-tagging working point
1-tag category:
- event does not fall into the 2-tag category
- one jet passes a 60% efficient b-tagging working point
- boosted decision tree used to select the matching jet
DOI: 10.17182/hepdata.82818.v1/t2
title: "Table 2" of "Search for Higgs boson pair production in the $\gamma\gamma b\bar{b}$ final state with 13 TeV $pp$ collision data collected by the ATLAS experiment"

description: The 95% CL observed and expected limits on the Higgs boson pair cross-section in picobarn and as a multiple of the SM production cross-section. The expected 1 sigma CLs bands are also indicated.
description: CERN-LHC, ATLAS.
Limits on pair production of Higgs bosons in the final state where one Higgs boson decays to two photons and the other to a b-quark together with its antiparticle.
The search is based on 36.1 +/- 1.2 fb^{-1} of pp collisions at sqrt{s} = 13 TeV recorded in 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider.
Data include at least one b-tagged jet and two well-identified isolated photons.
The search is sensitive to both resonant and non-resonant production of Higgs boson pairs.
Preselection:
- 2 jets with pT &gt; 25 GeV and |eta| &lt; 2.5, not within DeltaR = 0.4 of an isolated photon candidate or DeltaR = 0.2 of an isolated electron candidate
- Among isolated photons take the two with highest pT and require ET &gt; 0.35 * m_gammagamma and ET &gt; 0.25 * m_gammagamma respectively
- 105 &lt; m_gammagamma &lt; 160 GeV
After this preselection, two further kinematic selections are defined.
Loose selection:
- jet1 pT &gt; 40 GeV, jet2 pT &gt; 25 GeV
- 80 &lt; m_jj &lt; 140 GeV
- |m_gammagamma - m_H| &lt; 4.7 GeV (resonant search only)
Tight selection:
- jet1 pT &gt; 100 GeV, jet2 pT &gt; 30 GeV
- 90 &lt; m_jj &lt; 140 GeV
- |m_gammagamma - m_H| &lt; 4.3 GeV (resonant search only)
For each of these selections, a 1-tag and 2-tag category are considered.
2-tag category:
- both jets pass a 70% efficient b-tagging working point
1-tag category:
- event does not fall into the 2-tag category
- one jet passes a 60% efficient b-tagging working point
- boosted decision tree used to select the matching jet
DOI: 10.17182/hepdata.82818.v1/t3
title: "Table 3" of "Search for Higgs boson pair production in the $\gamma\gamma b\bar{b}$ final state with 13 TeV $pp$ collision data collected by the ATLAS experiment"

description: Number of data events for the 1-tag category with the loose selection in bins of diphoton mass.
description: CERN-LHC, ATLAS.
Limits on pair production of Higgs bosons in the final state where one Higgs boson decays to two photons and the other to a b-quark together with its antiparticle.
The search is based on 36.1 +/- 1.2 fb^{-1} of pp collisions at sqrt{s} = 13 TeV recorded in 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider.
Data include at least one b-tagged jet and two well-identified isolated photons.
The search is sensitive to both resonant and non-resonant production of Higgs boson pairs.
Preselection:
- 2 jets with pT &gt; 25 GeV and |eta| &lt; 2.5, not within DeltaR = 0.4 of an isolated photon candidate or DeltaR = 0.2 of an isolated electron candidate
- Among isolated photons take the two with highest pT and require ET &gt; 0.35 * m_gammagamma and ET &gt; 0.25 * m_gammagamma respectively
- 105 &lt; m_gammagamma &lt; 160 GeV
After this preselection, two further kinematic selections are defined.
Loose selection:
- jet1 pT &gt; 40 GeV, jet2 pT &gt; 25 GeV
- 80 &lt; m_jj &lt; 140 GeV
- |m_gammagamma - m_H| &lt; 4.7 GeV (resonant search only)
Tight selection:
- jet1 pT &gt; 100 GeV, jet2 pT &gt; 30 GeV
- 90 &lt; m_jj &lt; 140 GeV
- |m_gammagamma - m_H| &lt; 4.3 GeV (resonant search only)
For each of these selections, a 1-tag and 2-tag category are considered.
2-tag category:
- both jets pass a 70% efficient b-tagging working point
1-tag category:
- event does not fall into the 2-tag category
- one jet passes a 60% efficient b-tagging working point
- boosted decision tree used to select the matching jet
DOI: 10.17182/hepdata.82818.v1/t4
title: "Table 4" of "Search for Higgs boson pair production in the $\gamma\gamma b\bar{b}$ final state with 13 TeV $pp$ collision data collected by the ATLAS experiment"

description: Number of data events for the 2-tag category with the loose selection in bins of diphoton mass.
description: CERN-LHC, ATLAS.
Limits on pair production of Higgs bosons in the final state where one Higgs boson decays to two photons and the other to a b-quark together with its antiparticle.
The search is based on 36.1 +/- 1.2 fb^{-1} of pp collisions at sqrt{s} = 13 TeV recorded in 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider.
Data include at least one b-tagged jet and two well-identified isolated photons.
The search is sensitive to both resonant and non-resonant production of Higgs boson pairs.
Preselection:
- 2 jets with pT &gt; 25 GeV and |eta| &lt; 2.5, not within DeltaR = 0.4 of an isolated photon candidate or DeltaR = 0.2 of an isolated electron candidate
- Among isolated photons take the two with highest pT and require ET &gt; 0.35 * m_gammagamma and ET &gt; 0.25 * m_gammagamma respectively
- 105 &lt; m_gammagamma &lt; 160 GeV
After this preselection, two further kinematic selections are defined.
Loose selection:
- jet1 pT &gt; 40 GeV, jet2 pT &gt; 25 GeV
- 80 &lt; m_jj &lt; 140 GeV
- |m_gammagamma - m_H| &lt; 4.7 GeV (resonant search only)
Tight selection:
- jet1 pT &gt; 100 GeV, jet2 pT &gt; 30 GeV
- 90 &lt; m_jj &lt; 140 GeV
- |m_gammagamma - m_H| &lt; 4.3 GeV (resonant search only)
For each of these selections, a 1-tag and 2-tag category are considered.
2-tag category:
- both jets pass a 70% efficient b-tagging working point
1-tag category:
- event does not fall into the 2-tag category
- one jet passes a 60% efficient b-tagging working point
- boosted decision tree used to select the matching jet
DOI: 10.17182/hepdata.82818.v1/t5
title: "Table 5" of "Search for Higgs boson pair production in the $\gamma\gamma b\bar{b}$ final state with 13 TeV $pp$ collision data collected by the ATLAS experiment"

description: Number of data events for the 1-tag category with the tight selection in bins of diphoton mass.
description: CERN-LHC, ATLAS.
Limits on pair production of Higgs bosons in the final state where one Higgs boson decays to two photons and the other to a b-quark together with its antiparticle.
The search is based on 36.1 +/- 1.2 fb^{-1} of pp collisions at sqrt{s} = 13 TeV recorded in 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider.
Data include at least one b-tagged jet and two well-identified isolated photons.
The search is sensitive to both resonant and non-resonant production of Higgs boson pairs.
Preselection:
- 2 jets with pT &gt; 25 GeV and |eta| &lt; 2.5, not within DeltaR = 0.4 of an isolated photon candidate or DeltaR = 0.2 of an isolated electron candidate
- Among isolated photons take the two with highest pT and require ET &gt; 0.35 * m_gammagamma and ET &gt; 0.25 * m_gammagamma respectively
- 105 &lt; m_gammagamma &lt; 160 GeV
After this preselection, two further kinematic selections are defined.
Loose selection:
- jet1 pT &gt; 40 GeV, jet2 pT &gt; 25 GeV
- 80 &lt; m_jj &lt; 140 GeV
- |m_gammagamma - m_H| &lt; 4.7 GeV (resonant search only)
Tight selection:
- jet1 pT &gt; 100 GeV, jet2 pT &gt; 30 GeV
- 90 &lt; m_jj &lt; 140 GeV
- |m_gammagamma - m_H| &lt; 4.3 GeV (resonant search only)
For each of these selections, a 1-tag and 2-tag category are considered.
2-tag category:
- both jets pass a 70% efficient b-tagging working point
1-tag category:
- event does not fall into the 2-tag category
- one jet passes a 60% efficient b-tagging working point
- boosted decision tree used to select the matching jet
DOI: 10.17182/hepdata.82818.v1/t10
title: "Table 10" of "Search for Higgs boson pair production in the $\gamma\gamma b\bar{b}$ final state with 13 TeV $pp$ collision data collected by the ATLAS experiment"

description: Number of data events for the 2-tag category with the tight selection in bins of four-body mass.
description: CERN-LHC, ATLAS.
Limits on pair production of Higgs bosons in the final state where one Higgs boson decays to two photons and the other to a b-quark together with its antiparticle.
The search is based on 36.1 +/- 1.2 fb^{-1} of pp collisions at sqrt{s} = 13 TeV recorded in 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider.
Data include at least one b-tagged jet and two well-identified isolated photons.
The search is sensitive to both resonant and non-resonant production of Higgs boson pairs.
Preselection:
- 2 jets with pT &gt; 25 GeV and |eta| &lt; 2.5, not within DeltaR = 0.4 of an isolated photon candidate or DeltaR = 0.2 of an isolated electron candidate
- Among isolated photons take the two with highest pT and require ET &gt; 0.35 * m_gammagamma and ET &gt; 0.25 * m_gammagamma respectively
- 105 &lt; m_gammagamma &lt; 160 GeV
After this preselection, two further kinematic selections are defined.
Loose selection:
- jet1 pT &gt; 40 GeV, jet2 pT &gt; 25 GeV
- 80 &lt; m_jj &lt; 140 GeV
- |m_gammagamma - m_H| &lt; 4.7 GeV (resonant search only)
Tight selection:
- jet1 pT &gt; 100 GeV, jet2 pT &gt; 30 GeV
- 90 &lt; m_jj &lt; 140 GeV
- |m_gammagamma - m_H| &lt; 4.3 GeV (resonant search only)
For each of these selections, a 1-tag and 2-tag category are considered.
2-tag category:
- both jets pass a 70% efficient b-tagging working point
1-tag category:
- event does not fall into the 2-tag category
- one jet passes a 60% efficient b-tagging working point
- boosted decision tree used to select the matching jet
DOI: 10.17182/hepdata.82818.v1/t11
title: "Table 11" of "Search for Higgs boson pair production in the $\gamma\gamma b\bar{b}$ final state with 13 TeV $pp$ collision data collected by the ATLAS experiment"

description: Expected and observed upper limits at the 95% CL on the cross-section of gluon-fusion initiated Higgs boson pair production as a function of $\kappa_{\lambda}$.
description: CERN-LHC, ATLAS.
Limits on pair production of Higgs bosons in the final state where one Higgs boson decays to two photons and the other to a b-quark together with its antiparticle.
The search is based on 36.1 +/- 1.2 fb^{-1} of pp collisions at sqrt{s} = 13 TeV recorded in 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider.
Data include at least one b-tagged jet and two well-identified isolated photons.
The search is sensitive to both resonant and non-resonant production of Higgs boson pairs.
Preselection:
- 2 jets with pT &gt; 25 GeV and |eta| &lt; 2.5, not within DeltaR = 0.4 of an isolated photon candidate or DeltaR = 0.2 of an isolated electron candidate
- Among isolated photons take the two with highest pT and require ET &gt; 0.35 * m_gammagamma and ET &gt; 0.25 * m_gammagamma respectively
- 105 &lt; m_gammagamma &lt; 160 GeV
After this preselection, two further kinematic selections are defined.
Loose selection:
- jet1 pT &gt; 40 GeV, jet2 pT &gt; 25 GeV
- 80 &lt; m_jj &lt; 140 GeV
- |m_gammagamma - m_H| &lt; 4.7 GeV (resonant search only)
Tight selection:
- jet1 pT &gt; 100 GeV, jet2 pT &gt; 30 GeV
- 90 &lt; m_jj &lt; 140 GeV
- |m_gammagamma - m_H| &lt; 4.3 GeV (resonant search only)
For each of these selections, a 1-tag and 2-tag category are considered.
2-tag category:
- both jets pass a 70% efficient b-tagging working point
1-tag category:
- event does not fall into the 2-tag category
- one jet passes a 60% efficient b-tagging working point
- boosted decision tree used to select the matching jet
DOI: 10.17182/hepdata.82818.v1/t6
title: "Table 6" of "Search for Higgs boson pair production in the $\gamma\gamma b\bar{b}$ final state with 13 TeV $pp$ collision data collected by the ATLAS experiment"

description: Number of data events for the 2-tag category with the tight selection in bins of diphoton mass.
description: CERN-LHC, ATLAS.
Limits on pair production of Higgs bosons in the final state where one Higgs boson decays to two photons and the other to a b-quark together with its antiparticle.
The search is based on 36.1 +/- 1.2 fb^{-1} of pp collisions at sqrt{s} = 13 TeV recorded in 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider.
Data include at least one b-tagged jet and two well-identified isolated photons.
The search is sensitive to both resonant and non-resonant production of Higgs boson pairs.
Preselection:
- 2 jets with pT &gt; 25 GeV and |eta| &lt; 2.5, not within DeltaR = 0.4 of an isolated photon candidate or DeltaR = 0.2 of an isolated electron candidate
- Among isolated photons take the two with highest pT and require ET &gt; 0.35 * m_gammagamma and ET &gt; 0.25 * m_gammagamma respectively
- 105 &lt; m_gammagamma &lt; 160 GeV
After this preselection, two further kinematic selections are defined.
Loose selection:
- jet1 pT &gt; 40 GeV, jet2 pT &gt; 25 GeV
- 80 &lt; m_jj &lt; 140 GeV
- |m_gammagamma - m_H| &lt; 4.7 GeV (resonant search only)
Tight selection:
- jet1 pT &gt; 100 GeV, jet2 pT &gt; 30 GeV
- 90 &lt; m_jj &lt; 140 GeV
- |m_gammagamma - m_H| &lt; 4.3 GeV (resonant search only)
For each of these selections, a 1-tag and 2-tag category are considered.
2-tag category:
- both jets pass a 70% efficient b-tagging working point
1-tag category:
- event does not fall into the 2-tag category
- one jet passes a 60% efficient b-tagging working point
- boosted decision tree used to select the matching jet
DOI: 10.17182/hepdata.82818.v1/t7
title: "Table 7" of "Search for Higgs boson pair production in the $\gamma\gamma b\bar{b}$ final state with 13 TeV $pp$ collision data collected by the ATLAS experiment"

description: Number of data events for the 1-tag category with the loose selection in bins of four-body mass.
description: CERN-LHC, ATLAS.
Limits on pair production of Higgs bosons in the final state where one Higgs boson decays to two photons and the other to a b-quark together with its antiparticle.
The search is based on 36.1 +/- 1.2 fb^{-1} of pp collisions at sqrt{s} = 13 TeV recorded in 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider.
Data include at least one b-tagged jet and two well-identified isolated photons.
The search is sensitive to both resonant and non-resonant production of Higgs boson pairs.
Preselection:
- 2 jets with pT &gt; 25 GeV and |eta| &lt; 2.5, not within DeltaR = 0.4 of an isolated photon candidate or DeltaR = 0.2 of an isolated electron candidate
- Among isolated photons take the two with highest pT and require ET &gt; 0.35 * m_gammagamma and ET &gt; 0.25 * m_gammagamma respectively
- 105 &lt; m_gammagamma &lt; 160 GeV
After this preselection, two further kinematic selections are defined.
Loose selection:
- jet1 pT &gt; 40 GeV, jet2 pT &gt; 25 GeV
- 80 &lt; m_jj &lt; 140 GeV
- |m_gammagamma - m_H| &lt; 4.7 GeV (resonant search only)
Tight selection:
- jet1 pT &gt; 100 GeV, jet2 pT &gt; 30 GeV
- 90 &lt; m_jj &lt; 140 GeV
- |m_gammagamma - m_H| &lt; 4.3 GeV (resonant search only)
For each of these selections, a 1-tag and 2-tag category are considered.
2-tag category:
- both jets pass a 70% efficient b-tagging working point
1-tag category:
- event does not fall into the 2-tag category
- one jet passes a 60% efficient b-tagging working point
- boosted decision tree used to select the matching jet
DOI: 10.17182/hepdata.82818.v1/t8
title: "Table 8" of "Search for Higgs boson pair production in the $\gamma\gamma b\bar{b}$ final state with 13 TeV $pp$ collision data collected by the ATLAS experiment"

description: Number of data events for the 2-tag category with the loose selection in bins of four-body mass.
description: CERN-LHC, ATLAS.
Limits on pair production of Higgs bosons in the final state where one Higgs boson decays to two photons and the other to a b-quark together with its antiparticle.
The search is based on 36.1 +/- 1.2 fb^{-1} of pp collisions at sqrt{s} = 13 TeV recorded in 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider.
Data include at least one b-tagged jet and two well-identified isolated photons.
The search is sensitive to both resonant and non-resonant production of Higgs boson pairs.
Preselection:
- 2 jets with pT &gt; 25 GeV and |eta| &lt; 2.5, not within DeltaR = 0.4 of an isolated photon candidate or DeltaR = 0.2 of an isolated electron candidate
- Among isolated photons take the two with highest pT and require ET &gt; 0.35 * m_gammagamma and ET &gt; 0.25 * m_gammagamma respectively
- 105 &lt; m_gammagamma &lt; 160 GeV
After this preselection, two further kinematic selections are defined.
Loose selection:
- jet1 pT &gt; 40 GeV, jet2 pT &gt; 25 GeV
- 80 &lt; m_jj &lt; 140 GeV
- |m_gammagamma - m_H| &lt; 4.7 GeV (resonant search only)
Tight selection:
- jet1 pT &gt; 100 GeV, jet2 pT &gt; 30 GeV
- 90 &lt; m_jj &lt; 140 GeV
- |m_gammagamma - m_H| &lt; 4.3 GeV (resonant search only)
For each of these selections, a 1-tag and 2-tag category are considered.
2-tag category:
- both jets pass a 70% efficient b-tagging working point
1-tag category:
- event does not fall into the 2-tag category
- one jet passes a 60% efficient b-tagging working point
- boosted decision tree used to select the matching jet