Search results for "Project"

showing 10 items of 3466 documents

Electron-ion physics with the LHeC

2015

The Large Hadron Electron Collider (LHeC) project is the proposal to use the existing LHC proton/ion beams and construct a new electron beam line to perform high-energy electron-proton/ion collisions. In this talk, we consider some of the physics topics that could be studied in the electron-ion mode. In particular, we estimate how much the current nuclear parton distribution fits could be improved with the deeply inelastic scattering measurements at the LHeC by including pseudodata into a global analysis. In addition, we discuss briefly other topics that would help to better understand some aspects of heavy-ion collisions, namely small-$x$ physics and hadron production with a nuclear target.

PhysicsParticle physicsLarge Hadron ColliderProton010308 nuclear & particles physicsHadronFOS: Physical sciencesPartonElectronInelastic scatteringDeep inelastic scattering01 natural scienceslaw.inventionNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)lawelectron-ion physics0103 physical sciencesLHeCLarge Hadron Electron Collider project010306 general physicsColliderNuclear Experiment
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Muon-pair production by atmospheric muons in cosmoALEPH

2006

Data from a dedicated cosmic ray run of the ALEPH detector were used in a study of muon trident production, i.e., muon pairs produced by muons. Here the overburden and the calorimeters are the target materials while the ALEPH time projection chamber provides the momentum measurements. A theoretical estimate of the muon trident cross section is obtained by developing a Monte Carlo simulation for muon propagation in the overburden and the detector. Two muon trident candidates were found to match the expected theoretical pattern. The observed production rate implies that the nuclear form factor cannot be neglected for muon tridents.

PhysicsParticle physicsMuonTime projection chamberPhysics::Instrumentation and DetectorsMonte Carlo methodDetectorForm factor (quantum field theory)General Physics and AstronomyCosmic rayNuclear physicsPair productionMuon colliderPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentParticle Physics - Experiment
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Calibration of a camera-projector monochromatic system

2015

Camera–projector systems are increasingly being used in many different applications, including object reconstruction. In recent years, a number of approaches have been proposed to calibrate such devices; in this paper a calibration method is presented which can be used with monochromatic systems. The method is based on open-source code, makes use of planar calibration patterns, is fully automatic, easy to use and fast. Additionally, no initial information regarding the camera interior orientation is needed, and both sensors (camera and projector) are fully calibrated during the process. The method is validated by a series of tests, where root mean square errors (RMSEs) in image space are ke…

PhysicsProjector calibration0202 electrical engineering electronic engineering information engineeringEarth and Planetary Sciences (miscellaneous)020207 software engineering020201 artificial intelligence & image processing02 engineering and technologyComputers in Earth SciencesEngineering (miscellaneous)HumanitiesCartographyComputer Science ApplicationsThe Photogrammetric Record
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An intrinsic characterization of 2+2 warped spacetimes

2010

We give several equivalent conditions that characterize the 2+2 warped spacetimes: imposing the existence of a Killing-Yano tensor $A$ subject to complementary algebraic restrictions; in terms of the projector $v$ (or of the canonical 2-form $U$) associated with the 2-planes of the warped product. These planes are principal planes of the Weyl and/or Ricci tensors and can be explicitly obtained from them. Therefore, we obtain the necessary and sufficient (local) conditions for a metric tensor to be a 2+2 warped product. These conditions exclusively involve explicit concomitants of the Riemann tensor. We present a similar analysis for the conformally 2+2 product spacetimes and give an invaria…

PhysicsPure mathematicsRiemann curvature tensorPhysics and Astronomy (miscellaneous)Degenerate energy levelsFOS: Physical sciencesProduct metricGeneral Relativity and Quantum Cosmology (gr-qc)Fixed pointGeneral Relativity and Quantum Cosmologylaw.inventionsymbols.namesakeProjectorlawsymbolsTensorAlgebraic numberInvariant (mathematics)
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Oscillatory Localization of Quantum Walks Analyzed by Classical Electric Circuits

2016

We examine an unexplored quantum phenomenon we call oscillatory localization, where a discrete-time quantum walk with Grover's diffusion coin jumps back and forth between two vertices. We then connect it to the power dissipation of a related electric network. Namely, we show that there are only two kinds of oscillating states, called uniform states and flip states, and that the projection of an arbitrary state onto a flip state is bounded by the power dissipation of an electric circuit. By applying this framework to states along a single edge of a graph, we show that low effective resistance implies oscillatory localization of the quantum walk. This reveals that oscillatory localization occ…

PhysicsQuantum PhysicsFOS: Physical sciencesState (functional analysis)Edge (geometry)Dissipation01 natural sciencesProjection (linear algebra)010305 fluids & plasmasQuantum mechanicsBounded function0103 physical sciencesQuantum walkStatistical physics010306 general physicsQuantum Physics (quant-ph)QuantumElectronic circuit
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Entanglement in Gaussian matrix-product states

2006

Gaussian matrix product states are obtained as the outputs of projection operations from an ancillary space of M infinitely entangled bonds connecting neighboring sites, applied at each of N sites of an harmonic chain. Replacing the projections by associated Gaussian states, the 'building blocks', we show that the entanglement range in translationally-invariant Gaussian matrix product states depends on how entangled the building blocks are. In particular, infinite entanglement in the building blocks produces fully symmetric Gaussian states with maximum entanglement range. From their peculiar properties of entanglement sharing, a basic difference with spin chains is revealed: Gaussian matrix…

PhysicsQuantum PhysicsStatistical Mechanics (cond-mat.stat-mech)GaussianFOS: Physical sciencesMathematical Physics (math-ph)Quantum entanglementQuantum PhysicsQuantum numberSquashed entanglementMultipartite entanglementAtomic and Molecular Physics and OpticsProjection (linear algebra)Matrix multiplicationsymbols.namesakeQuantum mechanicssymbolsQuantum Physics (quant-ph)Quantum information scienceCondensed Matter - Statistical MechanicsMathematical PhysicsOptics (physics.optics)Physics - Optics
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Decoherence effects in the Stern-Gerlach experiment using matrix Wigner functions

2016

We analyze the Stern-Gerlach experiment in phase space with the help of the matrix Wigner function, which includes the spin degree of freedom. Such analysis allows for an intuitive visualization of the quantum dynamics of the device. We include the interaction with the environment, as described by the Caldeira-Leggett model. The diagonal terms of the matrix provide us with information about the two components of the state that arise from interaction with the magnetic field gradient. In particular, from the marginals of these components, we obtain an analytical formula for the position and momentum probability distributions in the presence of decoherence that shows a diffusive behavior for l…

PhysicsQuantum decoherenceStern–Gerlach experimentQuantum dynamicsQuantum entanglement01 natural sciencesProjection (linear algebra)010305 fluids & plasmasMatrix (mathematics)Phase spaceQuantum mechanics0103 physical sciencesWigner distribution function010306 general physicsPhysical Review A
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First observation ofγrays emitted from excited states south-east ofSn132: Theπg9/2−1⊗νf7/2multiplet ofIn83132

2016

For the first time, the γ decay of excited states has been observed in a nucleus situated in the quadrant south-east of doubly magic Sn132, a region in which experimental information so far is limited to ground-state properties. Six γ rays with energies of 50, 86, 103, 227, 357, and 602 keV were observed following the β-delayed neutron emission from Cd85133, populated in the projectile fission of a U238 beam at the Radioactive Isotope Beam Factory at RIKEN within the EURICA project. The new experimental information is compared to the results of a modern realistic shell-model calculation, the first one in this region very far from stability, focusing in particular on the π0g9/2-1 - ν1f7/2 pa…

PhysicsRadionuclide010308 nuclear & particles physicsFissionProjectileNeutron emission01 natural sciencesNuclear physicsExcited state0103 physical sciencesNeutronAtomic physicsNuclear Experiment010306 general physicsMultipletScalingPhysical Review C
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EPM calculations of E2/M1 mixing ratios for even samarium isotopes 146–152Sm

1987

Abstract The M1 operator and the E2/M1 mixing ratios, Δ (E2/M1), are discussed in the framework of the extended phonon projection model (EPM). The model is applied to 146, 148, 150, 152 Sm to describe their M1 properties. Comparison is made between the EPM, the consistent- Q formalism (CQF) of the basic interacting-boson approximation (IBA-1) and the experimental Δ(E2/M1) data. Both theoretical approaches give reasonably good results and parameter systematics.

PhysicsSamariumProjection modelNuclear and High Energy PhysicsFormalism (philosophy of mathematics)chemistryIsotopePhononQuantum electrodynamicschemistry.chemical_elementThermodynamicsPhysics Letters B
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Stochastic models for heterogeneous relaxation: Application to inhomogeneous optical lineshapes

2001

Dynamic heterogeneity has often been modeled by assuming that a single-particle observable, fluctuating at a molecular scale, is influenced by its coupling to environmental variables fluctuating on a second, perhaps slower, time scale. Starting from the most simple Gaussian Markov process we model the exchange between 'slow' and 'fast' environments by treating the fluctuating single-particle variable as a projection from a higher-dimensional Markov process. The moments of the resulting stochastic process are calculated from the corresponding Master equations or Langevin equations, depending on the model. The calculations show the importance of the way to treat exchange processes. The result…

PhysicsScale (ratio)Stochastic processStochastic modellingGaussianCondensed Matter (cond-mat)Markov processFOS: Physical sciencesCondensed MatterCondensed Matter PhysicsProjection (linear algebra)Electronic Optical and Magnetic Materialssymbols.namesakeMaster equationMaterials ChemistryCeramics and CompositessymbolsStatistical physicsRelaxation (approximation)
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