Search results for "IPR"

showing 10 items of 1515 documents

Tests and developments of the PANDA Endcap Disc DIRC

2016

The PANDA experiment at the future Facility for Antiproton and Ion Research (FAIR) requires excellent particle identification. Two different DIRC detectors will utilize internally reflected Cherenkov light of charged particles to enable the separation of pions and kaons up to momenta of 4 GeV/c. The Endcap Disc DIRC will be placed in the forward endcap of PANDA's central spectrometer covering polar angles between 5° and 22°. Its final design is based on MCP-PMTs for the photon detection and an optical system made of fused silica. A new prototype has been investigated during a test beam at CERN in May 2015 and first results will be presented. In addition a new synthetic fused silica material…

PhysicsLarge Hadron ColliderSpectrometerPhysics::Instrumentation and Detectors010308 nuclear & particles physicsDetectorRadiation01 natural sciencesCharged particleParticle identificationNuclear physics0103 physical sciencesFacility for Antiproton and Ion ResearchHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsInstrumentationMathematical PhysicsCherenkov radiationJournal of Instrumentation
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2012

A new apparatus has been designed that aims at a direct precision measurement of the g-factor of a single isolated proton or antiproton in a Penning trap. We present a thorough discussion on the trap design and a method for the experimental trap optimization using a single stored proton. A first attempt at the g-factor determination has been made in a section of the trap with a magnetic bottle. The Larmor frequency of the proton has been measured with a relative uncertainty of 1.8◊10 6 and the magnetic moment has been determined with a relative uncertainty of 8.9◊10 6 . Ag-factor of 5.585696(50) has been obtained, which is in excellent agreement with previous measurements and predictions. F…

PhysicsLarmor precessionProtonMagnetic momentOrders of magnitude (temperature)General Physics and AstronomyPenning trapTrap (computing)Nuclear physicsAntiprotonPhysics::Atomic PhysicsIon trapAtomic physicsNuclear ExperimentNew Journal of Physics
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Generalized formulation and symmetry properties of reciprocal nonabsorbing polarization devices: Application to liquid-crystal displays

2000

We present a general formulation based on the Jones-matrix theory for reciprocal nonabsorbing polarization devices, including polarization interference filters and liquid-crystal displays. The development of this formulation is based on general symmetry conditions that relate the Jones matrix when the device is illuminated from the front side and from the back side. The application to liquid-crystal displays results in a constraint of the Jones-matrix elements, which represents a generalization of the existing models that explain their modulation properties.

PhysicsLiquid crystal devicesLiquid-crystal displayPolarization rotatorBirefringencebusiness.industryPolarization (waves)Atomic and Molecular Physics and OpticsElectronic Optical and Magnetic Materialslaw.inventionOpticslawComputer Vision and Pattern RecognitionCrystal opticsbusinessReciprocal
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Dynamical and current-induced Dzyaloshinskii-Moriya interaction: Role for damping, gyromagnetism, and current-induced torques in noncollinear magnets

2020

Both applied electric currents and magnetization dynamics modify the Dzyaloshinskii-Moriya interaction (DMI), which we call current-induced DMI (CIDMI) and dynamical DMI (DDMI), respectively. We report a theory of CIDMI and DDMI. The inverse of CIDMI consists in charge pumping by a time-dependent gradient of magnetization ${\ensuremath{\partial}}^{2}\mathbit{M}(\mathbit{r},t)/\ensuremath{\partial}\mathbit{r}\ensuremath{\partial}t$, while the inverse of DDMI describes the torque generated by ${\ensuremath{\partial}}^{2}\mathbit{M}(\mathbit{r},t)/\ensuremath{\partial}\mathbit{r}\ensuremath{\partial}t$. In noncollinear magnets, CIDMI and DDMI depend on the local magnetization direction. The re…

PhysicsMagnetization dynamicsCondensed matter physicsCondensed Matter - Mesoscale and Nanoscale PhysicsMagnetismInverseFOS: Physical sciences02 engineering and technology021001 nanoscience & nanotechnology01 natural sciencesCondensed Matter - Other Condensed MatterMagnetizationFerromagnetismReciprocity (electromagnetism)Magnet0103 physical sciencesMesoscale and Nanoscale Physics (cond-mat.mes-hall)ddc:530Electric current010306 general physics0210 nano-technologyOther Condensed Matter (cond-mat.other)
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A model for the mass-number independence of the antiproton annihilation on nuclei at low energies

2001

Abstract A simple model explaining the recently observed approximate independence of the annihilation cross section on light nuclei at low energies is proposed. The salient idea is based on the realization that the π s from the annihilation on a nucleon have energies in the region of the Δ (1232) resonance. The coherent propagation of these π s through the excitation of several Δ resonances results in a destructive interference explaining why the annihilation of antiprotons in nuclei is suppressed. This model suggests a very effective way to produce “ Δ matter” with several Δ resonances in interaction.

PhysicsMass numberNuclear physicsCross section (physics)Nuclear and High Energy PhysicsAnnihilationAntiprotonResonanceAtomic physicsNucleonRealization (systems)ExcitationPhysics Letters B
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A fast solver for nonlocal electrostatic theory in biomolecular science and engineering

2011

Biological molecules perform their functions surrounded by water and mobile ions, which strongly influence molecular structure and behavior. The electrostatic interactions between a molecule and solvent are particularly difficult to model theoretically, due to the forces' long range and the collective response of many thousands of solvent molecules. The dominant modeling approaches represent the two extremes of the trade-off between molecular realism and computational efficiency: all-atom molecular dynamics in explicit solvent, and macroscopic continuum theory (the Poisson or Poisson--Boltzmann equation). We present the first fast-solver implementation of an advanced nonlocal continuum theo…

PhysicsMolecular dynamicsReciprocity (electromagnetism)Molecular biophysicsNanofluidicsStatistical physicsPoisson's equationSolverPoisson–Boltzmann equationBoltzmann equationComputational physicsProceedings of the 48th Design Automation Conference
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Realizing total reciprocity violation in the phase for photon scattering

2017

Scientific reports 7, 43114 (2017). doi:10.1038/srep43114

PhysicsMultidisciplinary000ScatteringDetectorSynchrotron radiationANALYZERNUCLEAR-RESONANCE01 natural sciencesArticlePOLARIZER010305 fluids & plasmasScattering amplitudeSYNCHROTRON-RADIATIONQuantum mechanics0103 physical sciencesddc:000Rotational invariance[CHIM]Chemical SciencesScattering theoryOPTICS010306 general physicsQuantumQUANTUMReciprocity (cultural anthropology)
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Double-trap measurement of the proton magnetic moment at 0.3 parts per billion precision

2017

Precise knowledge of the fundamental properties of the proton is essential for our understanding of atomic structure as well as for precise tests of fundamental symmetries. We report on a direct high-precision measurement of the magnetic moment μp of the proton in units of the nuclear magneton μN. The result, μp = 2.79284734462 (±0.00000000082) μN, has a fractional precision of 0.3 parts per billion, improves the previous best measurement by a factor of 11, and is consistent with the currently accepted value. This was achieved with the use of an optimized double–Penning trap technique. Provided a similar measurement of the antiproton magnetic moment can be performed, this result will enable…

PhysicsMultidisciplinaryMagnetic momentProton010308 nuclear & particles physicsProton magnetic moment7. Clean energy01 natural sciencesSymmetry (physics)Nuclear physicsBaryonAntiprotonAntimatter0103 physical sciencesPräzisionsexperimente - Abteilung BlaumAtomic physics010306 general physicsNuclear magnetonScience
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A note on Δn ≠ 0 Stark transitions in hydrogenlike atoms

1992

In a gaseous helium or hydrogen target slow muons or antiprotons are captured into orbits with a high principal quantum number (n = 15 to 50) to form (μ− α)+ ions, (pα)+ ions, or (pp) atoms respectively. In the subsequent deexcitation process Stark mixing of the intermediary states plays an important role. The successful Mainz Cascade Model assumed Δn = 0 for the Stark transitions, although formally no such selection rule exists. This note examines the reasons why Δn ≠ 0 Stark transitions play only a negligible role in the deexcitation cascade.

PhysicsMuonHydrogenGeneral Physics and Astronomychemistry.chemical_elementIonsymbols.namesakeStark effectchemistryAntiprotonCascadePrincipal quantum numberPhysics::Atomic and Molecular ClusterssymbolsPhysics::Atomic PhysicsAtomic physicsNuclear ExperimentExotic atomAnnalen der Physik
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Switching Reciprocity On and Off in a Magneto-Optical X-Ray Scattering Experiment Using Nuclear Resonance ofα−Fe57Foils

2012

Reciprocity is when the scattering amplitude of wave propagation satisfies a symmetry property, connecting a scattering process with an appropriate reversed one. We report on an experiment using nuclear resonance scattering of synchrotron radiation, which demonstrates that magneto-optical materials do not necessarily violate reciprocity. The setting enables us to switch easily between reciprocity and its violation. In the latter case, the exhibited reciprocity violation is orders of magnitude larger than achieved by previous wave scattering experiments.

PhysicsMössbauer effectCondensed matter physicsScatteringWave propagationX-rayGeneral Physics and AstronomySynchrotron radiation01 natural sciences010305 fluids & plasmasScattering amplitudeReciprocity (electromagnetism)Quantum mechanics0103 physical sciencesScattering theory010306 general physicsPhysical Review Letters
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