0000000000499307

AUTHOR

G. Martinez

showing 8 related works from this author

<title>Studies of the activation background in CsI(Tl) detectors</title>

1993

CsI scintillation crystals are widely used as detection in (gamma) -ray astronomy observations. In the MeV energy region, one of the most important background sources in CsI is the (beta) decays induced in the crystal by cosmic ray protons and their secondaries. One recent idea for reducing this background is to use discrete detector arrays to reject the large amount of localized (beta) decay events. Two experiments were carried out with 1 cm3 CsI crystals bombarded with energetic proton beams and fast/thermal neutrons, with the aim of evaluating the effectiveness of this method in pixelated (1 cm3) CsI detectors. The ratio of the number of decays resulting in single site and multiple site …

Nuclear physicsPhysicsScintillationPhotonProtonPhysics::Instrumentation and DetectorsDetectorSpallationCosmic rayNeutronNuclear ExperimentNeutron temperatureSPIE Proceedings
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Search forBs0→μ+μ−andB0→μ+μ−Decays with CDF II

2011

A search has been performed for B{sub s}{sup 0} {yields} {mu}{sup +}{mu}{sup -} and B{sup 0} {yields} {mu}{sup +}{mu}{sup -} decays using 7 fb{sup -1} of integrated luminosity collected by the CDF II detector at the Fermilab Tevatron collider. The observed number of B{sup 0} candidates is consistent with background-only expectations and yields an upper limit on the branching fraction of {Beta}(B{sup 0} {yields} {mu}{sup +}{mu}{sup -}) < 6.0 x 10{sup -9} at 95% confidence level. We observe an excess of B{sub s}{sup 0} candidates. The probability that the background processes alone could produce such an excess or larger is 0.27%. The probability that the combination of background and the expe…

Flight directionNuclear and High Energy PhysicsParticle physicsMesonTevatronGeneral Physics and Astronomy01 natural sciences7. Clean energyLuminosityStandard Modellaw.inventionNuclear physicsParticle decaychemistry.chemical_compoundlawTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITY0103 physical sciencesInvariant massLimit (mathematics)FermilabCollider010306 general physicsPhysicsMuon010308 nuclear & particles physicsBranching fractionSupersymmetryD0 experimentIMesCrystallographychemistryDecay lengthHigh Energy Physics::ExperimentLeptonPhysical Review Letters
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Measurement of thett¯production cross section inpp¯collisions ats=1.96  TeVusing soft electronb-tagging

2010

The authors present a measurement of the t{bar t} production cross section using events with one charged lepton and jets from p{bar p} collisions at a center-of-mass energy of 1.96 TeV. A b-tagging algorithm based on the probability of displaced tracks coming from the event interaction vertex is applied to identify b quarks from top decay. Using 318 pb{sup -1} of data collected with the CDF II detector, they measure the t{bar t} production cross section in events with at least one restrictive (tight) b-tagged jet and obtain 8.9{sub -1.0}{sup +1.0}(stat.){sub -1.0}{sup +1.1}(syst.) pb. The cross section value assumes a top quark mass of m{sub t} is presented in the paper. This result is cons…

Top quarkCollider physicsHadronTevatronGeneral Physics and AstronomyElementary particleKinematicsElectronJet (particle physics)01 natural sciences7. Clean energyParticle identificationlaw.inventionlawInvariant massFermilabNuclear ExperimentQuantum chromodynamicsPhysicsLarge Hadron ColliderLuminosity (scattering theory)Supersymmetryb-taggingHadronizationTransverse planeProduction (computer science)Collider Detector at FermilabQuarkSemileptonic decayNuclear and High Energy PhysicsParticle physicsBar (music)Astrophysics::High Energy Astrophysical PhenomenaBottom quarkMeasure (mathematics)Standard ModelNuclear physicsCross section (physics)Particle decay0103 physical sciencesCollider010306 general physicsCompact Muon SolenoidMuonBranching fraction010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyMultiplicity (mathematics)FermionVertex (geometry)Pair productionHigh Energy Physics::ExperimentEnergy (signal processing)Bar (unit)LeptonPhysical Review D
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MONSTER: a TOF Spectrometer for beta-delayed Neutron Spectroscopy

2014

β-delayed neutron (DN) data, including emission probabilities, Pn, and energy spectrum, play an important role in our understanding of nuclear structure, nuclear astrophysics and nuclear technologies. A MOdular Neutron time-of-flight SpectromeTER (MONSTER) is being built for the measurement of the neutron energy spectra and branching ratios. The TOF spectrometer will consist of one hundred liquid scintillator cells covering a significant solid angle. The MONSTER design has been optimized by using Monte Carlo (MC) techniques. The response function of the MONSTER cell has been characterized with mono-energetic neutron beams and compared to dedicated MC simulations.

PhysicsNuclear and High Energy PhysicsSpectrometerta114Nuclear TheoryNeutron stimulated emission computed tomographyNeutron scatteringNeutron temperatureNeutron time-of-flight scatteringNeutron spectroscopyNuclear physicsNeutron cross sectionNeutronNuclear ExperimentNuclear Data Sheets
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Global, regional, and national progress towards Sustainable Development Goal 3.2 for neonatal and child health: all-cause and cause-specific mortalit…

2021

Background: Sustainable Development Goal 3.2 has targeted elimination of preventable child mortality, reduction of neonatal death to less than 12 per 1000 livebirths, and reduction of death of children younger than 5 years to less than 25 per 1000 livebirths, for each country by 2030. To understand current rates, recent trends, and potential trajectories of child mortality for the next decade, we present the Global Burden of Diseases, Injuries, and Risk Factors Study (GBD) 2019 findings for all-cause mortality and cause-specific mortality in children younger than 5 years of age, with multiple scenarios for child mortality in 2030 that include the consideration of potential effects of COVID-…

MalePerinatal careNewborn careSTILLBIRTHSRJ101UNDER-5 MORTALITYPsychological intervention010501 environmental sciencesInfant mortalityGlobal Health01 natural sciences0302 clinical medicineRA0421Cause of DeathInfant MortalityGlobal healthLife TablesHealthcare improvements030212 general & internal medicine610 Medicine &amp; healthChildCause of Death; Child; COVID-19; Global Health; Humans; Infant; Life Tables; SARS-CoV-2; Sustainable Development11 Medical and Health SciencesCause of deathLife TableMortality rate1. No povertyPublic Health Global Health Social Medicine and EpidemiologyGeneral MedicineArticlesHälsovetenskaperSustainable DevelopmentMortality analyses3. Good healthPeer reviewChild PreschoolSDG 1 - No PovertyChild MortalityFemaleLife Sciences & BiomedicineHumanChild mortalityCOUNTRIESDEATHSInfants -- MortalitatGBD610 Medicine & health03 medical and health sciencesMedicine General & InternalSDG 3 - Good Health and Well-beingLife tablesunder-5 mortality rateGeneral & Internal MedicineHealth SciencesNeonatal deathsmedicineSYSTEMATIC ANALYSISHumans:Medicine [Science]Infants -- SalutPreschool0105 earth and related environmental sciencesScience & TechnologyInfants nadons -- Salutbusiness.industrySARS-CoV-2Infants nadons -- MortalitatINFORMInfant NewbornCOVID-19InfantNeonatal and child health ; Sustainable Development Goal 3.2 ; Global healthGBD 2019 Under-5 Mortality Collaboratorsmedicine.diseaseNewbornTRENDSInfant mortalitySustainable Development GoalChild mortalityFolkhälsovetenskap global hälsa socialmedicin och epidemiologiDeaths3121 General medicine internal medicine and other clinical medicineRGbusinessSystematic AnalysisMalariaDemography
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CCDC 832986: Experimental Crystal Structure Determination

2012

Related Article: P.A.Ochoa, S.Delgado, A.Gallego, C.J.Gomez-Garcia, R.Jimenez-Aparicio, G.Martinez, J.Perles, M.R.Torres|2012|Inorg.Chem.|51|5844|doi:10.1021/ic3004307

Space GroupCrystallographyCrystal SystemCrystal StructureCell Parameterscatena-(hexakis(mu~3~-Propionato)-bis(mu~2~-propionato)-tetrakis(mu~2~-cyano)-di-gold-tetra-rhodium-di-potassium)Experimental 3D Coordinates
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CCDC 832982: Experimental Crystal Structure Determination

2012

Related Article: P.A.Ochoa, S.Delgado, A.Gallego, C.J.Gomez-Garcia, R.Jimenez-Aparicio, G.Martinez, J.Perles, M.R.Torres|2012|Inorg.Chem.|51|5844|doi:10.1021/ic3004307

Space GroupCrystallographyCrystal SystemCrystal StructureCell Parameterstetrakis(mu~2~-propanoato)-diaqua-di-rhodiumExperimental 3D Coordinates
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CCDC 832987: Experimental Crystal Structure Determination

2012

Related Article: P.A.Ochoa, S.Delgado, A.Gallego, C.J.Gomez-Garcia, R.Jimenez-Aparicio, G.Martinez, J.Perles, M.R.Torres|2012|Inorg.Chem.|51|5844|doi:10.1021/ic3004307

Space GroupCrystallographyCrystal SystemCrystal StructureCell Parameterscatena-(tris(mu~3~-Acetato)-(mu~3~-cyano)-(mu~2~-acetato)-(mu~2~-cyano)-triaqua-gold-di-rhodium-potassium monohydrate)Experimental 3D Coordinates
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