Search results for "Integra"

showing 10 items of 5314 documents

Rubidium dimers in paraffin-coated cells

2010

Measurements were made to determine the density of rubidium dimer vapor in paraffin-coated cells. The number density of dimers and atoms in similar paraffin-coated and uncoated cells was measured by optical spectroscopy. Due to the relatively low melting point of paraffin, a limited temperature range of 43-80 deg C was explored, with the lower end corresponding to a dimer density of less than 10^7 cm^(-3). With one-minute integration time, a sensitivity to dimer number density of better than 10^6 cm^(-3) was achieved. No significant difference in dimer density was observed between the cells.

Time delay and integrationPhysicsQuantum PhysicsNumber densityAtomic Physics (physics.atom-ph)DimerSignificant differenceAnalytical chemistryGeneral Physics and Astronomychemistry.chemical_elementLow melting pointFOS: Physical sciences02 engineering and technologyAtmospheric temperature range021001 nanoscience & nanotechnology01 natural sciencesPhysics - Atomic PhysicsRubidiumchemistry.chemical_compoundchemistry0103 physical sciences010306 general physics0210 nano-technologySpectroscopyQuantum Physics (quant-ph)
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Stiffness-Adaptive Taylor method for the integration of non-stiff and stiff kinetic models

1992

A systematic derivation procedure that greatly facilitates the application of the Taylor method to the integration of kinetic models is developed. In addition, an algorithm that gives the integration step as a function of the required level of accuracy is proposed. Using the Taylor method, application of this algorithm is immediate and largely reduces the integration time. In addition, a new method of integration of kinetic models, whose most important feature is the self-adaptability to the stiffness of the system along the integration process, is developed. This “stiffness-adaptive” Taylor method (SAT method) makes use of several algorithms, combining them to meet the particular requireme…

Time delay and integrationProcess (engineering)MathematicsofComputing_NUMERICALANALYSISStiffnessGeneral ChemistryFunction (mathematics)Kinetic energyDerivation procedureComputational MathematicsTaylor methodFeature (computer vision)medicinemedicine.symptomAlgorithmMathematicsJournal of Computational Chemistry
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High performance algorithms based on a new wawelet expansion for time dependent acoustics obstale scattering

2007

This paper presents a highly parallelizable numerical method to solve time dependent acoustic obstacle scattering problems. The method proposed is a generalization of the ``operator expansion method" developed by Recchioni and Zirilli [SIAM J.~Sci.~Comput., 25 (2003), 1158-1186]. The numerical method proposed reduces, via a perturbative approach, the solution of the scattering problem to the solution of a sequence of systems of first kind integral equations. The numerical solution of these systems of integral equations is challenging when scattering problems involving realistic obstacles and small wavelengths are solved. A computational method has been developed to solve these challenging p…

Time dependent acoustic scattering Helmholtz equation integral equation methodswavelet bases sparse linear systems
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Boundedness and compactness of operators related to time-frequency analysis

2018

En esta tesis, estudiamos diferentes aspectos de los operadores relacionados con el análisis tiempo-frecuencia. Cada operador lineal y continuo de la clase de Schwartz en su dual, el espacio de distribuciones temperadas, se puede escribir como un operador integral con núcleo K, o también como un operador integral de Fourier (de hecho, pseudodiferencial). Las diferentes condiciones en el núcleo o el símbolo y la fase (en el caso de los operadores integrales de Fourier) permiten extender el operador a varios espacios de funciones y distribuciones. A continuación detallamos los contenidos de la memoria. En el primer capítulo presentamos la notación, las definiciones de algunos espacios, de suc…

Time-frequency analysisFourier integral operatorsGabor Frames:MATEMÁTICAS::Análisis y análisis funcional [UNESCO]UNESCO::MATEMÁTICAS::Análisis y análisis funcional
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Biodegradation of differently cross-linked collagen membranes: an experimental study in the rat.

2005

Contains fulltext : 47774.pdf (Publisher’s version ) (Closed access) The aim of the present study was to compare the biodegradation of differently cross-linked collagen membranes in rats. Five commercially available and three experimental membranes (VN) were included: (1) BioGide (BG) (non-cross-linked porcine type I and III collagens), (2) BioMend (BM), (3) BioMendExtend (BME) (glutaraldehyde cross-linked bovine type I collagen), (4) Ossix (OS) (enzymatic-cross-linked bovine type I collagen), (5) TutoDent (TD) (non-cross-linked bovine type I collagen, and (6-8) VN(1-3) (chemical cross-linked porcine type I and III collagens). Specimens were randomly allocated in unconnected subcutaneous po…

Tissue engineering and reconstructive surgery [UMCN 4.3]Time FactorsSwineForeign-Body ReactionBovine Type I CollagenTissue integrationCollagen membraneMembranes ArtificialAnatomyBiodegradationRatsAndrologychemistry.chemical_compoundMembranechemistryAbsorbable ImplantsAnimalsAnimal studyCattleGlutaraldehydeCollagenOral SurgeryRats Wistar
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Search for a heavy top-quark partner in final states with two leptons with the ATLAS detector at the LHC

2012

The results of a search for direct pair production of heavy top-quark partners in 4.7 fb[superscript −1] of integrated luminosity from pp collisions at s√ = 7 TeV collected by the ATLAS detector at the LHC are reported. Heavy top-quark partners decaying into a top quark and a neutral non-interacting particle are searched for in events with two leptons in the final state. No excess above the Standard Model expectation is observed. Limits are placed on the mass of a supersymmetric scalar top and of a spin-1/2 top-quark partner. A spin-1/2 top-quark partner with a mass between 300 GeV and 480 GeV, decaying to a top quark and a neutral non-interacting particle lighter than 100 GeV, is excluded …

Top quark01 natural sciences7. Clean energyHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear ExperimentQCPhysicsddc:539Large Hadron ColliderLuminosity (scattering theory)[SDU.ASTR.HE]Sciences of the Universe [physics]/Astrophysics [astro-ph]/High Energy Astrophysical Phenomena [astro-ph.HE]Settore FIS/01 - Fisica SperimentaleSupersymmetryATLASComputer Science::Computers and Societyhmedicine.anatomical_structurehadron-hadronComputingMethodologies_DOCUMENTANDTEXTPROCESSINGFísica nuclearLHCParticle Physics - ExperimentParticle physicsNuclear and High Energy Physics[PHYS.ASTR.HE]Physics [physics]/Astrophysics [astro-ph]/High Energy Astrophysical Phenomena [astro-ph.HE]leptonsCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]FOS: Physical sciences530Standard ModelNuclear physicsAtlas (anatomy)0103 physical sciencesmedicinePhysics::Atomic and Molecular Clustersddc:530High Energy Physics010306 general physicsCiencias ExactasHadron-Hadron scattering; Nuclear and High Energy PhysicsHadron-Hadron ScatteringScience & TechnologyATLAS detector010308 nuclear & particles physicsscatteringHigh Energy Physics::PhenomenologyFísicaPair productionNonlinear Sciences::Exactly Solvable and Integrable SystemsHADRON-HADRON COLLISIONSExperimental High Energy PhysicsHigh Energy Physics::ExperimentsupersymmetryLeptonhadron-hadron; hadron-hadron scattering; scattering
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Search for anomalous top-quark couplings with the D0 detector

2008

Anomalous Wtb couplings modify the angular correlations of the top quark decay products and change the single top quark production cross section. We present limits on anomalous top quark couplings by combining information from W boson helicity measurements in top quark decays and anomalous coupling searches in the single top quark final state. We set limits on right-handed vector couplings as well as left-handed and right-handed tensor couplings based on about 1fb^-1 of data collected by the D0 experiment.

Top quarkParticle physicsInfrared fixed pointHigh Energy Physics::LatticeGeneral Physics and AstronomyFOS: Physical sciences01 natural sciencesBottom quarkHigh Energy Physics - ExperimentNuclear physicsParticle decayHigh Energy Physics - Experiment (hep-ex)0103 physical sciencesPhysics::Atomic and Molecular Clusters[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]B meson010306 general physics14.65.Ha; 12.15.Ji; 13.85.QkPhysicsCoupling010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTop quark condensateHelicityNonlinear Sciences::Exactly Solvable and Integrable SystemsHigh Energy Physics::Experiment
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Cross-section-constrained top-quark mass measurement from dilepton events at the tevatron

2008

We report the first top quark mass measurement that uses a cross section constraint to improve the mass determination. This measurement is made with a dilepton $t\bar{t}$ event sample collected with the CDF II detector. From a data sample corresponding to an integrated luminosity of 1.2 fb$^{-1}$, we measure a top quark mass of $\rm{170.7^{+4.2}_{-3.9}(stat)\pm2.6(syst)}$ $\rm{\pm2.4(theory) GeV/{\it{c}}^{2}}$. The measurement without the cross section constraint results in a top quark mass of $\rm{169.7^{+5.2}_{-4.9}(stat)\pm3.1(syst) GeV/{\it{c}}^{2}}$.

Top quarkParticle physicsPhysics MultidisciplinaryTevatronFOS: Physical sciencesGeneral Physics and Astronomyddc:500.2Molecular dynamics01 natural sciencesHigh Energy Physics - Experimentlaw.inventionNuclear physicsHigh Energy Physics - Experiment (hep-ex)Colliding beam acceleratorslaw0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]FermilabHigh energy physicsNuclear Experiment010306 general physicsColliderConstraint theoryAstrophysics::Galaxy AstrophysicsPhysicsLuminosity (scattering theory)010308 nuclear & particles physicsPhysicsHigh Energy Physics::PhenomenologyDetector14.65.Ha 13.85.Ni 13.85.Qk 12.15.FfIntegrated controlConstraint (information theory)Collider DetectorFermi levelCross-section constraintsHigh Energy Physics::ExperimentEvent (particle physics)Top-quark mass measurement
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LEM for twisted re-entrant angle sections

2014

In this paper an innovative numerical method named as line element-less method, LEM, for finding solution of torsion problem has been extended to all shaped sections, including sections possessing re-entrant angles at their boundary. The response solution in terms of shear stress field or Prandtl function or warping function in all domain and for any kind of domain with arbitrary contour, may be performed quickly, calculating line integrals only. The method takes full advantage of the theory of analytic complex function and is robust in the sense that returns exact solution if this exists. Numerical implementation of LEM has been developed using Mathematica software without resorting to any…

TorsionRe-entrant angleDiscretizationMechanical EngineeringNumerical analysisMathematical analysisPrandtl numberLine integralTorsion (mechanics)GeometryStress fieldComputer Science ApplicationsStress fieldsymbols.namesakeExact solutions in general relativityModeling and SimulationShear stresssymbolsComplex potential functionGeneral Materials ScienceCivil and Structural EngineeringMathematicsComputers & Structures
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Fazioni e popolo in una provincia del dominio pontificio fra XIII e XIV secolo

2021

Between the 13th and 14th centuries, a number of cities in the inchoative papal state experimented a system of self-government that allowed the Guelph and Ghibelline factions, formally represented in those same bodies on an equal footing, to work alongside the more strictly communal magistracies. The case of Todi is rather well known, given the role that Bartolo da Sassoferrato assigns to it in his Tractatus de guelphis et gebellinis (ca. 1350), but current research has already ascertained that this political tradition appeared at least around 1260. Some evidence can suggest, however, that some form of integration of factions into the local institutional framework was possible elsewhere, an…

Tra XIII e XIV secolo alcune città dello stato della chiesa in formazione sperimentano un regime di autogoverno che prevede accanto agli organi più propriamente comunali la presenza delle fazioni guelfa e ghibellina formalmente rappresentate in quegli stessi organi in modo paritario. Il caso di Todi è piuttosto noto data la funzione che Bartolo da Sassoferrato gli assegna nel suo Tractatus de guelphis et gebellinis (1350 circa) ma la storiografia ha già appurato che questa tradizione politica durava dal 1260 circa almeno. Alcuni indizi fanno ritenere che però la possibilità di una qualche forma di integrazione delle fazioni nel quadro istituzionale locale avvenisse anche altrove e non lontano ad Amelia a esempio. Qui nel nuovo statuto di popolo 1343 troviamo la ripartizione su base fazionaria dei ruoli del priorato. A Todi nel 1337 era avvenuto qualcosa di analogo: lo statuto emanato quell’anno fa seguito all’instaurazione di un regime esplicitamente popolare che in continuità con la tradizione locale integra al suo interno guelfi e ghibellini. Gli esempi di queste e forse altre comunità della provincia del Patrimonio di san Pietro in Tuscia possono così aggiungere qualche elemento utile alla discussione sul problema delle fazioni e del loro ruolo nell’ordine politico comunale e post-comunale e in particolare sul rapporto fra popolo come sistema istituzionale e parti.Settore M-STO/01 - Storia Medievale
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