0000000001266815

AUTHOR

A Meyer

showing 3 related works from this author

Using the Multidimensional Prognostic Index to Predict Clinical Outcomes of Hospitalized Older Persons: A Prospective, Multicenter, International Stu…

2018

Abstract Background Multidimensional Prognostic Index (MPI) is useful as a prognostic tool in hospitalized older patients, but our knowledge is derived from retrospective studies. We therefore aimed to evaluate in a multicenter, longitudinal, cohort study whether the MPI at hospital admission is useful to identify groups with different mortality risk and whether MPI at discharge may predict institutionalization, rehospitalization, and use of home care services during 12 months. Methods This longitudinal study, carried out between February 2015 and August 2017, included nine public hospitals in Europe and Australia. A standardized comprehensive geriatric assessment including information on f…

MaleAgingmedicine.medical_specialtyLongitudinal studyIndex (economics)InstitutionalisationPrognosi030204 cardiovascular system & hematologyRisk Assessment03 medical and health sciencesHospital0302 clinical medicinePredictive Value of TestsMultidimensional Prognostic IndexmedicineRisk of mortalityHumansLongitudinal StudiesProspective Studies030212 general & internal medicineGeriatric AssessmentAgedAged 80 and overbusiness.industryAustraliaRetrospective cohort studyOdds ratioPrognosisEuropeHospitalizationROC CurveThe Journal of Gerontology: Medical SciencesEmergency medicineCohortFemaleGeriatrics and GerontologybusinessCohort studyCohort study
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Higgs boson studies at the Tevatron

2013

We combine searches by the CDF and D0 Collaborations for the standard model Higgs boson with mass in the range 90-200 GeV/c2 produced in the gluon-gluon fusion, WH, ZH, tt̄H, and vector boson fusion processes, and decaying in the H→bb̄, H→W+W-, H→ZZ, H→τ+τ-, and H→γγ modes. The data correspond to integrated luminosities of up to 10 fb-1 and were collected at the Fermilab Tevatron in pp̄ collisions at √s=1.96 TeV. The searches are also interpreted in the context of fermiophobic and fourth generation models. We observe a significant excess of events in the mass range between 115 and 140 GeV/c2. The local significance corresponds to 3.0 standard deviations at mH=125 GeV/c2, consistent with the…

FERMILAB TEVATRON COLLIDERNuclear and High Energy PhysicsParticle physicsproton antiproton collisions; FERMILAB TEVATRON COLLIDER; Standard Model Higgs boson; BROKEN SYMMETRIESSTANDARD MODELP(P)OVER-BAR COLLISIONSTevatronFOS: Physical sciencesContext (language use)ATLAS DETECTORddc:500.2Standard Model Higgs boson7. Clean energy01 natural sciencesStandard ModelVector bosonHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)SEARCH0103 physical sciencesBibliography[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]BROKEN SYMMETRIESFermilab010306 general physicsPhysicsHIGGS BOSONB-JET IDENTIFICATIONLarge Hadron ColliderPP COLLISIONS010308 nuclear & particles physics4. EducationHigh Energy Physics::PhenomenologyROOT-S=1.96 TEVPARTON DISTRIBUTIONSExperimental High Energy PhysicsHiggs bosonproton antiproton collisionsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGSYMMETRIESCDFB-JET IDENTIFICATION; STANDARD MODEL; ATLAS DETECTOR; PP COLLISIONS; P(P)OVER-BAR COLLISIONS; PARTON DISTRIBUTIONS; ROOT-S=1.96 TEV; SEARCH; LHC; SYMMETRIESHigh Energy Physics::ExperimentLHC
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Combination of measurements of the top-quark pair production cross section from the Tevatron Collider

2014

We combine six measurements of the inclusive top-quark pair (tt̄) production cross section (σtt̄) from data collected with the CDF and D0 detectors at the Fermilab Tevatron with proton-antiproton collisions at s=1.96TeV. The data correspond to integrated luminosities of up to 8.8fb-1. We obtain a value of σtt̄=7.60±0.41pb for a top-quark mass of mt=172.5GeV. The contributions to the uncertainty are 0.20 pb from statistical sources, 0.29 pb from systematic sources, and 0.21 pb from the uncertainty on the integrated luminosity. The result is in good agreement with the standard model expectation of 7.35-0.33+0.28pb at next-to-next-to-leading order and next-to-next-to leading logarithms in pert…

Top quarkP(P)OVER-BAR COLLISIONSTevatron7. Clean energylaw.inventionPhysics Particles & FieldsHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)law[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]HADRON COLLIDERSFERMILABFermilabNuclear ExperimentQuantum chromodynamicsPhysicsLarge Hadron ColliderPhysicsP(P)OVER-BAR COLLISIONS; ROOT-S=1.96 TEV; PARTON DISTRIBUTIONS; HADRON COLLIDERS; LEADING ORDER; T(T)OVER-BAR; DETECTOR; LHC; QCD; FERMILABPerturbative QCD3. Good healthROOT-S=1.96 TEVPhysical SciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSINGLHCT(T)OVER-BARParticle physicsNuclear and High Energy PhysicsFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic AstrophysicsAstronomy & AstrophysicsMASSNuclear physicsSEARCHColliderParticle PhysicsDETECTORAstrophysics::Galaxy AstrophysicsScience & Technologyhep-exLEADING ORDERHigh Energy Physics::PhenomenologyTop quarkQCDP(P)OVER-BAR COLLISIONS; T(T)OVER-BAR; DETECTOR; SEARCH; MASSPair productionPARTON DISTRIBUTIONSExperimental High Energy PhysicsCollider PhysicsCDFHigh Energy Physics::ExperimentParticle Physics; Collider Physics; Top quark
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