Search results for "Tellurium"

showing 10 items of 135 documents

Rydberg and autoionizing states of tellurium studied by laser resonance ionization spectroscopy

2019

Multistep laser-resonance-ionization spectroscopy of tellurium (Te) has been performed at TRIUMF's off-line laser ion source test stand. Six clean and regular even-parity Rydberg series $5{p}^{3}$ $({^{4}S}_{3/2}^{\ensuremath{\circ}})$ $np\phantom{\rule{4pt}{0ex}}^{3}P_{0,1,2}$, $np\phantom{\rule{4pt}{0ex}}^{5}P_{1,2}$, and $nf\phantom{\rule{4pt}{0ex}}^{3}F_{2}/^{5}F_{1,2}$ were observed. The ionization potential of Te was extracted from the measured series as $72669.114{(56)}_{\mathrm{stat}}{(45)}_{\mathrm{sys}}\phantom{\rule{4pt}{0ex}}{\mathrm{cm}}^{\ensuremath{-}1}$. Excited from two different intermediate levels, seven odd-parity autoionization Rydberg series converging to the $5{s}^{2}…

Physicschemistry.chemical_element01 natural sciences3. Good health010305 fluids & plasmassymbols.namesakechemistryAutoionizationExcited stateIonization0103 physical sciencesRydberg formulasymbolsLaser resonanceAtomic physicsIonization energy010306 general physicsSpectroscopyTelluriumPhysical Review A
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Potentialities of High-Resolution 3-D CZT Drift Strip Detectors for Prompt Gamma-Ray Measurements in BNCT

2022

Recently, new high-resolution cadmium–zinc–telluride (CZT) drift strip detectors for room temperature gamma-ray spectroscopic imaging were developed by our group. The CZT detectors equipped with orthogonal anode/cathode collecting strips, drift strips and dedicated pulse processing allow a detection area of 6 × 20 mm2 and excellent room temperature spectroscopic performance (0.82% FWHM at 661.7 keV). In this work, we investigated the potentialities of these detectors for prompt gamma-ray spectroscopy (PGS) in boron neutron capture therapy (BNCT). The detectors, exploiting the measurement of the 478 keV prompt gamma rays emitted by 94% 7Li nuclides from the 10B(n, α)7…

Physics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaSettore FIS/01 - Fisica SperimentalePhysics::Medical PhysicsBNCT; CZT detectors; X-ray and gamma-ray detectorsBoron Neutron Capture TherapyCZT detectors; X-ray and gamma-ray detectors; BNCTBiochemistrySettore FIS/07 - Fisica Applicata(Beni Culturali Ambientali Biol.e Medicin)Atomic and Molecular Physics and OpticsAnalytical ChemistryZincX-ray and gamma-ray detectorsGamma RaysBNCTTelluriumElectrical and Electronic EngineeringInstrumentationCadmiumCZT detectors
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A measurement of material in the ATLAS tracker using secondary hadronic interactions in 7 TeV pp collisions

2016

Knowledge of the material in the ATLAS inner tracking detector is crucial in understanding the reconstruction of charged-particle tracks, the performance of algorithms that identify jets containing b-hadrons and is also essential to reduce background in searches for exotic particles that can decay within the inner detector volume. Interactions of primary hadrons produced in pp collisions with the material in the inner detector are used to map the location and amount of this material. The hadronic interactions of primary particles may result in secondary vertices, which in this analysis are reconstructed by an inclusive vertex-finding algorithm. Data were collected using minimum-bias trigger…

Physics::Instrumentation and DetectorsCiencias FísicasHadronsecondary [vertex]01 natural sciencesHigh Energy Physics - Experiment//purl.org/becyt/ford/1 [https]High Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]scattering [p p]of photons with matter interaction of hadrons with matter etc)tracking detectorInstrumentationGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)Mathematical PhysicsQCPhysicsDetector modelling and simulations I (interaction of radiation with matter interaction of photons with matter interaction of hadrons with matter etc)Performance of high energy physics detectorsLarge Hadron ColliderAtlas (topology)DetectorSettore FIS/01 - Fisica Sperimentaleexotic [particle]ATLAStrackingprimary [vertex]CERN LHC CollDetector modelling and simulations I (interaction of radiation with matter interaction of photons with matter interaction of hadrons with matter etc); Performance of High Energy Physics DetectorsAtlasTellurium compoundsParticle Physics - ExperimentperformanceCIENCIAS NATURALES Y EXACTASParticle physics530 PhysicsCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]Detector modelling and simulations I (interaction of radiation with matter interactionFOS: Physical sciencesLHC ATLAS High Energy Physics530MaterialNuclear physics510 Mathematics0103 physical sciencesddc:610High Energy Physics010306 general physicsCiencias ExactasScience & Technology010308 nuclear & particles physicstracks [charged particle]backgroundFísica//purl.org/becyt/ford/1.3 [https]triggerAstronomíaExperimental High Energy PhysicsHigh Energy Physics::Experimenthadron
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Search for the Associated Production of the Standard-Model Higgs Boson in the All-Hadronic Channel

2009

We report on a search for the standard-model Higgs boson in pp collisions at s=1.96 TeV using an integrated luminosity of 2.0 fb(-1). We look for production of the Higgs boson decaying to a pair of bottom quarks in association with a vector boson V (W or Z) decaying to quarks, resulting in a four-jet final state. Two of the jets are required to have secondary vertices consistent with B-hadron decays. We set the first 95% confidence level upper limit on the VH production cross section with V(-> qq/qq('))H(-> bb) decay for Higgs boson masses of 100-150 GeV/c(2) using data from run II at the Fermilab Tevatron. For m(H)=120 GeV/c(2), we exclude cross sections larger than 38 times the standard-m…

QuarkParticle physicsStandardsFinal stateFermilab TevatronHiggs bosonTevatronFOS: Physical sciencesGeneral Physics and AstronomyElementary particleddc:500.201 natural sciences114 Physical sciencesStandard ModelVector bosonHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Particle decayTellurium compounds0103 physical sciencesJetsB-hadron decaysHigh energy physics010306 general physicsBosonsBosonStandard-model Higgs bosonsPhysicsIntegrated luminosityHIGGS BOSONModel predictionCross section010308 nuclear & particles physicsPhysicsHigh Energy Physics::PhenomenologyConfidence levelsUpper limits3. Good healthVector bosonProduction cross sectionBottom quarksSecondary verticesHiggs bosonCDFHigh Energy Physics::Experiment
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Combination of the Searches for Pair-Produced Vectorlike Partners of the Third-Generation Quarks at s=13  TeV with the ATLAS Detector

2018

A combination of the searches for pair-produced vectorlike partners of the top and bottom quarks in various decay channels (T -> Zt/Wb/Ht, B -> Zb/Wt/Hb) is performed using 36.1 fb(-1) of pp ...

QuarkPhysicsParticle physicsLarge Hadron Collider010308 nuclear & particles physicsAtlas detectorGeneral Physics and AstronomyElementary particle01 natural sciencesThird generation3. Good healthmedicine.anatomical_structureAtlas (anatomy)Isospin0103 physical sciencesmedicine010306 general physicsTellurium compoundsPhysical Review Letters
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First measurement of the charge asymmetry in beauty-quark pair production.

2014

The difference in the angular distributions between beauty quarks and antiquarks, referred to as the charge asymmetry, is measured for the first time in b[bar over b] pair production at a hadron collider. The data used correspond to an integrated luminosity of 1.0  fb[superscript −1] collected at 7 TeV center-of-mass energy in proton-proton collisions with the LHCb detector. The measurement is performed in three regions of the invariant mass of the b[bar over b] system. The results obtained are A[b[bar over b] over C](40 105  GeV/c[superscript 2]) = 1.6 ± 1.7 ± 0.6%, where A[b[bar over b] over C] is defined as the asymmetry in the difference in rapidity between jets formed from the beauty q…

ROOT-S=7 TEV; COLLISIONS; DETECTOR; DECAYcharge asymmetriesGeneral Physics and Astronomy7. Clean energyHigh Energy Physics - ExperimentSettore FIS/04 - Fisica Nucleare e Subnuclearehigh energy physicsthe standard model[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]photonsInvariant massNuclear ExperimentQCmedia_commonPhysicsLarge Hadron Colliderhadron collidersintegrated luminosityParticle physicsroot-S=7 Tev; colisions; detector; decayFísica nuclearLHCtellurium compoundsParticle Physics - ExperimentQuarkCOLLISIONSParticle physics530 Physicsmedia_common.quotation_subjectPhysics InstituteLHCb - Abteilung HofmannBottom quarkAsymmetryStandard ModelNuclear physicsPhysics and Astronomy (all)RapiditySDG 7 - Affordable and Clean EnergyDETECTOR14.65.Fyhadron colliders; tellurium compounds; center-of-mass energies; transverse planes; charge asymmetries; integrated luminosity; high energy physics; pair production; photons; the standard model; proton proton collisions/dk/atira/pure/sustainabledevelopmentgoals/affordable_and_clean_energyROOT-S=7 TEVcenter-of-mass energiesHigh Energy Physics::PhenomenologyBottom quarkproton proton collisionsLHCbpair productionPair productiontransverse planesHigh Energy Physics::ExperimentFísica de partículesExperimentsDECAYPhysical review letters
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Growth and characterisation of MnTe crystals

2001

We report on the low temperature growth of MnTe crystals by means of travelling solution methods. Two different processes are considered; a classical THM process using a low temperature presynthesised MnTe ingot, and a modified THM process, in which an increasing length of solvent zone collects the tellurium that was added to the stoichiometric charge to decrease the reaction temperature. Ingots from the two methods are analysed by means of scanning electron microscopy, X-ray diffractometry, resistivity, susceptibility and optical absorption measurements.

Scanning electron microscopeAnalytical chemistrychemistry.chemical_elementCondensed Matter PhysicsMagnetic susceptibilityInorganic ChemistrySolventCrystallographychemistryElectrical resistivity and conductivityMaterials ChemistryAbsorption (chemistry)IngotTelluriumStoichiometryJournal of Crystal Growth
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CCDC 711250: Experimental Crystal Structure Determination

2010

Related Article: J.L.Dutton, H.M.Tuononen, P.J.Ragogna|2009|Angew.Chem.,Int.Ed.|48|4409|doi:10.1002/anie.200901495

Space GroupCrystallographyCrystal SystemCrystal StructureCell Parameters(12-bis(26-Di-isopropylphenylimino)acenaphthene-NN')-bis(trifluoromethanesulfonato-O)-tellurium(ii) dichloromethane solvateExperimental 3D Coordinates
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CCDC 143980: Experimental Crystal Structure Determination

2001

Related Article: H.Fleischer, D.Schollmeyer|2000|Angew.Chem.,Int.Ed.|39|3705|doi:10.1002/1521-3773(20001016)39:20<3705::AID-ANIE3705>3.0.CO;2-Y

Space GroupCrystallographyCrystal SystemCrystal StructureCell ParametersAqua-bis(2-hydroxyethanethiolato)-tellurium(ii)Experimental 3D Coordinates
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CCDC 173863: Experimental Crystal Structure Determination

2002

Related Article: H.Fleischer, B.Mathiasch, D.Schollmeyer|2002|Organometallics|21|526|doi:10.1021/om0104159

Space GroupCrystallographyCrystal SystemCrystal StructureCell ParametersTrichloro-(2-chloro-3-hydroxypropyl-CO)-tellurium dichloro-(2-chloro-3-oxypropyl-CO)-telluriumExperimental 3D Coordinates
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