Search results for "2HDM"

showing 8 items of 138 documents

"Table 89: Mass distribution, 2 tag, mbb window 510" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in th…

2018

The mass distribution of the llbb system used in the fit to derive the limits for the mbb window centered at 510 GeV for the nb = 2 (2 tag) category.

Z0 --> MU+ MU-Z0 --> E+ E-2HDMP P --> HIGGSHIGGS --> BQ BQBAR13000.0gluon-gluon fusionmass distributionb-associated productionMHiggs boson productionHIGGS --> Z0 HIGGSgluon fusion
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"Table 118: Mass distribution, 3 tag, mbb window 650" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in t…

2018

The mass distribution of the llbb system used in the fit to derive the limits for the mbb window centered at 650 GeV for the nb >= 3 (3 tag) category.

Z0 --> MU+ MU-Z0 --> E+ E-2HDMP P --> HIGGSHIGGS --> BQ BQBAR13000.0gluon-gluon fusionmass distributionb-associated productionMHiggs boson productionHIGGS --> Z0 HIGGSgluon fusion
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"Table 44: Mass distribution, 3 tag, mbb window 260" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in th…

2018

The mass distribution of the llbb system used in the fit to derive the limits for the mbb window centered at 260 GeV for the nb >= 3 (3 tag) category.

Z0 --> MU+ MU-Z0 --> E+ E-2HDMP P --> HIGGSHIGGS --> BQ BQBAR13000.0gluon-gluon fusionmass distributionb-associated productionMHiggs boson productionHIGGS --> Z0 HIGGSgluon fusion
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"Table 120: Mass distribution, 3 tag, mbb window 660" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in t…

2018

The mass distribution of the llbb system used in the fit to derive the limits for the mbb window centered at 660 GeV for the nb >= 3 (3 tag) category.

Z0 --> MU+ MU-Z0 --> E+ E-2HDMP P --> HIGGSHIGGS --> BQ BQBAR13000.0gluon-gluon fusionmass distributionb-associated productionMHiggs boson productionHIGGS --> Z0 HIGGSgluon fusion
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"Table 105: Mass distribution, 2 tag, mbb window 590" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in t…

2018

The mass distribution of the llbb system used in the fit to derive the limits for the mbb window centered at 590 GeV for the nb = 2 (2 tag) category.

Z0 --> MU+ MU-Z0 --> E+ E-2HDMP P --> HIGGSHIGGS --> BQ BQBAR13000.0gluon-gluon fusionmass distributionb-associated productionMHiggs boson productionHIGGS --> Z0 HIGGSgluon fusion
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"Table 36: Mass distribution, 3 tag, mbb window 220" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in th…

2018

The mass distribution of the llbb system used in the fit to derive the limits for the mbb window centered at 220 GeV for the nb >= 3 (3 tag) category.

Z0 --> MU+ MU-Z0 --> E+ E-2HDMP P --> HIGGSHIGGS --> BQ BQBAR13000.0mass distributiongluon-gluon fusionb-associated productionMHiggs boson productionHIGGS --> Z0 HIGGSgluon fusion
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"Table 2" of "Search for Higgs boson decays into a $Z$ boson and a light hadronically decaying resonance using 13 TeV $pp$ collision data from the AT…

2020

Efficiencies of the MLP selection, complete selection and total expected signal yields for each signal sample, assuming B$(H\to Z(Q/a))=100\%$ and $\sigma(pp\to H) = \sigma_\text{SM}(pp\to H)$. Pythia 8 branching fractions of $a$ are assumed using a $\tan\beta$ value of 1. The MLP efficiencies, total efficiencies, and expected yields are determined using MC samples, with uncertainties due to MC sample statistics, except for the expected background yield. The expected background yield and its uncertainty is calculated as described in the main text of the paper.

p p ---> t tbarYields13000.0p p ---> Z Zp p ---> H ---> Z JpsiHiggs bosonp p ---> H ---> Z etac2HDM(+S)p p ---> H ---> Z aATLASp p ---> Z jetEfficienciesProton-Proton ScatteringLHCp p ---> W Z
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"Table 1" of "Search for Higgs boson decays into a $Z$ boson and a light hadronically decaying resonance using 13 TeV $pp$ collision data from the AT…

2020

Observed number of data events and expected number of background events in the signal region.

p p ---> t tbarp p ---> e e jet13000.0p p ---> Z ZProton-Proton ScatteringHiggs bosonEvents2HDM(+S)p p ---> mu mu jetLHCATLASp p ---> W Zp p ---> Z jet
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