Search results for "Linear"

showing 10 items of 7165 documents

The fixed angle scattering problem with a first order perturbation

2021

We study the inverse scattering problem of determining a magnetic field and electric potential from scattering measurements corresponding to finitely many plane waves. The main result shows that the coefficients are uniquely determined by $2n$ measurements up to a natural gauge. We also show that one can recover the full first order term for a related equation having no gauge invariance, and that it is possible to reduce the number of measurements if the coefficients have certain symmetries. This work extends the fixed angle scattering results of Rakesh and M. Salo to Hamiltonians with first order perturbations, and it is based on wave equation methods and Carleman estimates.

PhysicsNuclear and High Energy Physicsinverse scattering problemsScattering010102 general mathematicsMathematical analysisPlane waveInverseFOS: Physical sciencesStatistical and Nonlinear PhysicsMathematical Physics (math-ph)Gauge (firearms)Wave equation01 natural sciencesinversio-ongelmat010101 applied mathematicsMathematics - Analysis of PDEsInverse scattering problemFOS: MathematicsGauge theoryElectric potential0101 mathematicsMathematical PhysicsAnalysis of PDEs (math.AP)
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Character of particle-hole excitations in94Ru deduced fromγ-ray angular correlation and linear polarization measurements

2014

Linear polarization and angular correlations of gamma-rays depopulating excited states in the neutron-deficient nucleus Ru-94(44)50 have been measured, enabling firm spin-parity assignments for several excited states in this nucleus. The deduced multipolarities of strong transitions in the yrast structure were found to be mostly of stretched M1, E1, and E2 types and, in most cases, in agreement with previous tentative assignments. The deduced multipolarity of the 1869 keV and the connecting 257 and 1641 keV transitions indicates that the state at 6358 keV excitation energy has spin parity 12(1)(-) rather than 12(3)(+) as proposed in previous works. The presence of a 12(1)(-) state is interp…

PhysicsNuclear and High Energy Physicsmedicine.anatomical_structureAngular correlationLinear polarizationExcited stateYrastmedicineNeutronParity (physics)Atomic physicsNucleusExcitationPhysical Review C
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Spinrotator for MAMI

1991

A source of polarized electrons based on the photoemission of a GaAsP-cathode [1] has been set up to inject polarized electrons in the Mainz microtron MAMI. In order to compensate the spin precession in MAMI a spinrotator system has to be integrated in the 100 keV beamline from the source to the injector linac to achieve the required longitudinal spin direction at target position.

PhysicsNuclear physicsBeamlinePhysics::Instrumentation and DetectorsPrecessionPhysics::Accelerator PhysicsCondensed Matter::Strongly Correlated ElectronsElectronNuclear ExperimentSpin (physics)Precession angleMicrotronLinear particle accelerator
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INVESTIGATION OF FAR-INFRARED SMITH-PURCELL RADIATION AT THE 3.41 MEV ELECTRON INJECTOR LINAC OF THE MAINZ MICROTRON MAMI

2006

PhysicsNuclear physicsFar infraredlawCathode rayInjectorElectronRadiationMicrotronLinear particle acceleratorlaw.invention
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Photonuclear reactions induced by a clinical linac

2015

1st NUBA International Conference on Nuclear Physics and Astrophysics -- SEP 14-21, 2014 -- Akdeniz Univ, Antalya, TURKEY

PhysicsNuclear physicsHistoryIrradiation[0-Belirlenecek]Beam (structure)Bremsstrahlung photonLinear particle accelerator3. Good healthComputer Science ApplicationsEducationSemiconductor detectorJournal of Physics: Conference Series
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Relations between polarization observables and complete sets for deuteron photodisintegration

1990

The polarization observables for deuteron photodisintegration are given as Hermitean forms of theT-matrix elementsti. By inversion we are able to express a given productti*tj in terms of polarization observables. This allows (i) to derive linear relations between observables for unpolarized, circularly and linearly polarized photons, (ii) to construct explicitly complete sets of polarization observables, and (iii) to derive quadratic relations between observables.

PhysicsNuclear physicsParticle physicsPhotonQuadratic equationDeuteriumLinear polarizationPhotodisintegrationPolarization observablesObservableAtomic and Molecular Physics and OpticsFew-Body Systems
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Corrections for positon annihilation in flight in nuclear spectrometry

1973

Abstract Theories of positon single- and two-quanta annihilation in flight, the Fermi beta-decay theory, and theories of positon energy loss are used in calculations of total probabilities of annihilation in flight of positons in continuous spectra. The results are given in a nomogram useful in correcting for positon annihilation in flight in various nuclear-spectrometry experiments. Confirmation of the theoretical basis employed was obtained by comparing total absolute probabilities for annihilation in flight of 62 Cu positons in Perspex, copper, cadmium and lead, using a new differential method. The agreement with the theory was found to be excellent. A method for obtaining “correct” posi…

PhysicsNuclear physicsScintillationNonlinear Sciences::Exactly Solvable and Integrable SystemsAnnihilationContinuous spectrumGamma spectroscopyGeneral MedicineAtomic physicsSpectroscopySpectral lineSemiconductor detectorFermi Gamma-ray Space TelescopeNuclear Instruments and Methods
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Die elektronenstreu-apparatur am mainzer 300 MeV-elektronen-linearbeschleuniger

1972

Abstract In this paper, we attempt to give a general survey and a comprehensive description of the most significant features of the facilities for electron scattering experiments at the Mainz 300 MeV Linear Accelerator, along with a list of literature, where more detailed information on certain subjects can be found. The accelerator provides energies between 80 and 300 MeV. Scattering angles are available up to 160° resulting in a momentum transfer region up to 3.0 fm −1 . The overall experimental resolution is 0.1%. Cross sections down to 10 −34 cm 2 /sr can be measured. The main features of the apparatus are: an achromatic magnet system with 90° deflection, a double focusing spectrometer,…

PhysicsNuclear physicsSpectrometerAchromatic lenslawScatteringMomentum transferGeneral MedicineElectronElectron scatteringLinear particle acceleratorBeam (structure)law.inventionNuclear Instruments and Methods
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The Pion Single-Event Latch-Up Cross Section Enhancement: Mechanisms and Consequences for Accelerator Hardness Assurance

2021

Pions make up a large part of the hadronic environment typical of accelerator mixed fields. Characterizing device cross sections against pions is usually disregarded in favor of tests with protons, whose single-event latch-up (SEL) cross section is, nonetheless, experimentally found to be lower than that of pions for all energies below 250 MeV. While Monte Carlo simulations are capable of reproducing such behavior, the reason for the observed pion cross-section enhancement can only be explained by a deeper analysis of the underlying mechanisms dominating proton–silicon and pion–silicon reactions. The mechanisms dominating the SEL response are found to vary with the energy under consideratio…

PhysicsNuclear reactionNuclear and High Energy PhysicsMesonNuclear TheoryMonte Carlo methodHadronLinear energy transfer02 engineering and technology021001 nanoscience & nanotechnologyAccelerators and Storage Rings01 natural sciences7. Clean energyNuclear physicsCross section (physics)PionNuclear Energy and Engineering0103 physical sciencesNuclear Physics - ExperimentHigh Energy Physics::ExperimentElectrical and Electronic EngineeringNuclear Experiment010306 general physics0210 nano-technologyEvent (particle physics)IEEE Transactions on Nuclear Science
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Nuclear structure of 157Gd

2003

Abstract The energy levels of 157 Gd have been investigated using the (n,  γ ) and (n, n′ γ ) reactions. As a result of the analysis of the γ -ray spectra from 16 isolated neutron resonances, a level scheme with a complete set of levels with spins J =1/2, 3/2 has been established up to 1.86 MeV excitation energy. A part of the level scheme is interpreted in more detail on the basis of Coriolis and Δ N =2 coupled Nilsson configurations. Slightly different sets of shape parameters are deduced for negative- and positive-parity levels. A large excess of unassigned 1/2 and 3/2 levels evidently requires an explanation in terms of inclusion of new additional degrees of freedom.

PhysicsNuclear reactionNuclear and High Energy PhysicsSpinsBasis (linear algebra)Degrees of freedom (physics and chemistry)Nuclear structureNeutronAtomic physicsExcitationSpectral lineNuclear Physics A
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