Search results for "MANIPULATION"

showing 10 items of 311 documents

Hermite interpolation: The barycentric approach

1991

The barycentric formulas for polynomial and rational Hermite interpolation are derived; an efficient algorithm for the computation of these interpolants is developed. Some new interpolation principles based on rational interpolation are discussed.

Numerical AnalysisMathematical analysisComputingMethodologies_IMAGEPROCESSINGANDCOMPUTERVISIONMathematicsofComputing_NUMERICALANALYSISTrilinear interpolationStairstep interpolationBirkhoff interpolationComputer Science ApplicationsTheoretical Computer SciencePolynomial interpolationComputational MathematicsComputational Theory and MathematicsNearest-neighbor interpolationHermite interpolationComputingMethodologies_SYMBOLICANDALGEBRAICMANIPULATIONApplied mathematicsSpline interpolationSoftwareComputingMethodologies_COMPUTERGRAPHICSMathematicsInterpolationComputing
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Numerical Study of Two Sparse AMG-methods

2003

A sparse algebraic multigrid method is studied as a cheap and accurate way to compute approximations of Schur complements of matrices arising from the discretization of some symmetric and positive definite partial differential operators. The construction of such a multigrid is discussed and numerical experiments are used to verify the properties of the method.

Numerical AnalysisMathematical optimizationDiscretizationApplied MathematicsNumerical analysisMathematicsofComputing_NUMERICALANALYSISPositive-definite matrixFinite element methodComputational MathematicsMultigrid methodModeling and SimulationComputingMethodologies_SYMBOLICANDALGEBRAICMANIPULATIONSchur complementApplied mathematicsPartial derivativeAnalysisMathematicsSparse matrixESAIM: Mathematical Modelling and Numerical Analysis
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Mellin transform approach for the solution of coupled systems of fractional differential equations

2015

In this paper, the solution of a multi-order, multi-degree-of-freedom fractional differential equation is addressed by using the Mellin integral transform. By taking advantage of a technique that relates the transformed function, in points of the complex plane differing in the value of their real part, the solution is found in the Mellin domain by solving a linear set of algebraic equations. The approximate solution of the differential (or integral) equation is restored, in the time domain, by using the inverse Mellin transform in its discretized form.

Numerical AnalysisMellin transformLaplace transformApplied MathematicsMathematical analysisMulti degree of freedom systemsRamanujan's master theoremIntegral equationFractional differential equationWiener–Hopf methodsymbols.namesakeModeling and SimulationLaplace transform applied to differential equationsComputingMethodologies_SYMBOLICANDALGEBRAICMANIPULATIONsymbolsMellin inversion theoremTwo-sided Laplace transformMellin transformMathematicsCommunications in Nonlinear Science and Numerical Simulation
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Walsh function analysis of 2-D generalized continuous systems

1990

The importance of the generalized or singular 2D continuous systems are demonstrated by showing their use in the solution of partial differential equations in two variables. A technique is presented for solving these systems in terms of Walsh functions. The method replaces the solution of a two-variable partial differential equation with the solution of a linear algebraic generalized 2D Sylvester equation. An efficient technique for the recursive solution of the latter equation is offered. All the results apply also in the usual Roesser 2D state-space case. >

Partial differential equationDifferential equationWeak solutionMathematical analysisMathematicsofComputing_NUMERICALANALYSISFirst-order partial differential equationParabolic partial differential equationComputer Science ApplicationsMethod of characteristicsControl and Systems EngineeringComputingMethodologies_SYMBOLICANDALGEBRAICMANIPULATIONElectrical and Electronic EngineeringSylvester equationUniversal differential equationMathematicsIEEE Transactions on Automatic Control
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Singular distributed parameter systems

1993

The paper deals with the distributed parameter systems described by coupled partial differential equations with singular matrix coefficients. Initial-boundary-value problems are considered in the light of both singular 1d systems theory and the Fourier approach to distributed parameter systems. The method presented in this paper gives the possibility of determining acceptable initial-boundary conditions. An illustrative example is given.

Partial differential equationMathematical analysisGeneral EngineeringSeparation principlesymbols.namesakeFourier transformSystems theoryDistributed parameter systemSingular solutionComputingMethodologies_SYMBOLICANDALGEBRAICMANIPULATIONsymbolsInitial value problemBoundary value problemMathematicsIEE Proceedings D Control Theory and Applications
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Assessment of Tumor Development and Wound Healing Using Endoscopic Techniques in Mice

2010

Mouse models of intestinal inflammation and colon cancer are valuable tools to gain insights into the pathogenesis of the corresponding human diseases. Recently, in vivo mouse endoscopy has been developed, allowing not only the high-resolution monitoring and scoring of experimental disease development, but also enables the investigator to perform manipulations, including local injection of reagents or the taking of biopsies for molecular and histopathologic analyses. Chromoendoscopic staining with methylene blue enables visualization of the crypt structure and allows discrimination between inflammatory and neoplastic changes. The development of endoscopic techniques in live mice opened new …

Pathologymedicine.medical_specialtyColorectal cancerBiopsyDiseasePathogenesisMiceMicromanipulation03 medical and health sciences0302 clinical medicineIn vivoIntestinal inflammationmedicineAnimalsHumans030304 developmental biologyWound Healing0303 health sciencesMiniaturizationHepatologymedicine.diagnostic_testbusiness.industryDisease mechanismsGastroenterologyEndoscopyColitismedicine.disease3. Good healthEndoscopyEndoscopes GastrointestinalDisease Models AnimalColonic Neoplasms030211 gastroenterology & hepatologybusinessWound healingGastroenterology
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Roadmap on STIRAP applications

2019

STIRAP (stimulated Raman adiabatic passage) is a powerful laser-based method, usually involving two photons, for efficient and selective transfer of populations between quantum states. A particularly interesting feature is the fact that the coupling between the initial and the final quantum states is via an intermediate state, even though the lifetime of the latter can be much shorter than the interaction time with the laser radiation. Nevertheless, spontaneous emission from the intermediate state is prevented by quantum interference. Maintaining the coherence between the initial and final state throughout the transfer process is crucial. STIRAP was initially developed with applications in …

PhotonAtomic Physics (physics.atom-ph)Digital storageStimulated Raman adiabatic passage02 engineering and technologyStimulated Raman adiabatic passage (STIRAP)01 natural scienceslaw.inventionPhysics - Atomic PhysicsFTIR SPECTROSCOPYstimulated Raman adiabatic passage (STIRAP)lawStereochemistryRare earthsStatistical physicsMetal ionsmolecular Rydberg statesQCparity violationPhysicseducation.field_of_studyQuantum PhysicsElectric dipole momentsCoherent population transfer021001 nanoscience & nanotechnologyCondensed Matter Physicsacoustic waves; molecular Rydberg states; nuclear coherent population transfer; parity violation; spin waves; stimulated Raman adiabatic passage (STIRAP); ultracold moleculesADIABATIC PASSAGEAtomic and Molecular Physics and OpticsChemical DynamicsMolecular beamsVIOLATING ENERGY DIFFERENCEResearch group A. Pálffy – Division C. H. KeitelStimulated emission0210 nano-technologyCoherence (physics)Experimental parametersPopulationFOS: Physical sciencesacoustic waves530spin wavesMolecular Rydberg statesELECTROMAGNETICALLY INDUCED TRANSPARENCYSINGLE PHOTONSQuantum statePhysics - Chemical Physics0103 physical sciencesUltracold moleculesSpontaneous emissionddc:530Nuclear coherent population transfer010306 general physicseducationStimulated Raman adiabatic passageChemical Physics (physics.chem-ph)Rare-earth-ion doped crystalsPhotonsQuantum opticsnuclear coherent population transferBROAD-BANDControlled manipulationsPOLAR-MOLECULESMoleculesRydberg statesLaserSuperconducting quantum circuitAcoustic wavesParity violationstimulated Raman adiabatic passage (STIRAP); ultracold molecules; parity violation; spin waves; acoustic waves; molecular Rydberg states; nuclear coherent population transferDewey Decimal Classification::500 | Naturwissenschaften::530 | Physikultracold moleculesQuantum Physics (quant-ph)QUANTUM GASSpin waves
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"Table 1" of "Backward electroproduction of pi0 mesons on protons in the region of nucleon resonances at four momentum transfer squared Q**2 = 1.0-Ge…

2005

Cross section SIG(T) + EPSILON*SIG(L) for COS(THETA*) = -0.975.

Photoproduction1.11-1.95ComputingMilieux_THECOMPUTINGPROFESSIONElectron productionTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITYE- P --> E- P PI0ComputingMethodologies_SYMBOLICANDALGEBRAICMANIPULATIONMathematicsofComputing_NUMERICALANALYSISExclusiveInformationSystems_MISCELLANEOUSD2SIG/DOMEGADouble Differential Cross SectionGAMMA* P --> P PI0
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"Table 2" of "Backward electroproduction of pi0 mesons on protons in the region of nucleon resonances at four momentum transfer squared Q**2 = 1.0-Ge…

2005

Cross section SIG(T) + EPSILON*SIG(L) for COS(THETA*) = -0.925.

PhotoproductionComputingMilieux_THECOMPUTINGPROFESSIONElectron productionTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITYE- P --> E- P PI0ComputingMethodologies_SYMBOLICANDALGEBRAICMANIPULATION1.11-1.77MathematicsofComputing_NUMERICALANALYSISExclusiveInformationSystems_MISCELLANEOUSD2SIG/DOMEGADouble Differential Cross SectionGAMMA* P --> P PI0
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"Table 4" of "Backward electroproduction of pi0 mesons on protons in the region of nucleon resonances at four momentum transfer squared Q**2 = 1.0-Ge…

2005

Cross section SIG(T) + EPSILON*SIG(L) for COS(THETA*) = -0.825.

PhotoproductionComputingMilieux_THECOMPUTINGPROFESSIONElectron productionTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITYE- P --> E- P PI0ComputingMethodologies_SYMBOLICANDALGEBRAICMANIPULATIONMathematicsofComputing_NUMERICALANALYSIS1.11-1.45ExclusiveInformationSystems_MISCELLANEOUSD2SIG/DOMEGADouble Differential Cross SectionGAMMA* P --> P PI0
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