Search results for "Algorithms"

showing 10 items of 1716 documents

AGATA-Advanced GAmma Tracking Array

2012

WOS: 000300864200005

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsPulse-shape and gamma-ray tracking algorithmsFOS: Physical sciencesSemiconductor detector performance and simulationsIntegrated circuit[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Tracking (particle physics)gamma-Ray tracking01 natural sciencesPulse-shape and γ-ray tracking algorithmslaw.inventionData acquisitionlaw0103 physical sciencesddc:530[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Nuclear Experiment (nucl-ex)010306 general physicsγ-Ray spectroscopyNuclear ExperimentInstrumentationDigital signal processingEvent reconstructiongamma-Ray spectroscopyPhysicssezeleSpectrometerSpectrometers010308 nuclear & particles physicsbusiness.industryDetectorAGATA Digital signals HPGe detectors Pulse-shape Ray trackingHPGe detectorsAlgorithms Crystals Germanium Semiconductor detectors Signal processing Spectrometry Tracking (position)γ-Ray trackingInstrumentation and Detectors (physics.ins-det)Digital signal processingAGATAFísica nuclearbusinessAGATAComputer hardware
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Particle identification with COMPASS RICH-1

2011

International audience; RICH-1 is a large size RICH detector in operation at the COMPASS experiment since 2001 and recently upgraded implementing a new photon detection system with increased performance.A dedicated software package has been developed to perform RICH-1 data reduction, pattern recognition and particle identification as well as a number of accessory tasks for detector studies.The software package, the algorithms implemented and the detector characterisation and performance are reported in detail.

Nuclear and High Energy PhysicsPhysics::Instrumentation and Detectors[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesCOMPASSParticle identificationParticle identificationCompass0103 physical sciencesCOMPASS experimentComputer vision010306 general physicsInstrumentationRICHPhysics010308 nuclear & particles physicsbusiness.industryDetectorSoftware packageParticle identification; COMPASS; Likelihood algorithmsPattern recognition (psychology)High Energy Physics::ExperimentArtificial intelligenceLikelihood algorithmsbusinessPhoton detectionData reduction
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Sensitivity enhancement in pulse EPR distance measurements

2004

Established pulse EPR approaches to the measurement of small dipole-dipole couplings between electron spins rely on constant-time echo experiments to separate relaxational contributions from dipolar time evolution. This requires a compromise between sensitivity and resolution to be made prior to the measurement, so that optimum data are only obtained if the magnitude of the dipole-dipole coupling is known beforehand to a good approximation. Moreover, the whole dipolar evolution function is measured with relatively low sensitivity. These problems are overcome by a variable-time experiment that achieves suppression of the relaxation contribution by reference deconvolution. Theoretical and exp…

Nuclear and High Energy PhysicsProtein ConformationBiophysicsAnalytical chemistryBiochemistrySensitivity and Specificitylaw.inventionlawspin labelingSensitivity (control systems)protein structurepair correlation functionElectron paramagnetic resonanceCouplingSpinsChemistryPulsed EPRRelaxation (NMR)Time evolutionElectron Spin Resonance SpectroscopyPhotosystem II Protein ComplexReproducibility of ResultsSignal Processing Computer-AssistedELDORCondensed Matter PhysicsComputational physicsDeconvolutionEPRAlgorithms
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Correcting for Potential Barriers in Quantum Walk Search

2015

A randomly walking quantum particle searches in Grover's $\Theta(\sqrt{N})$ iterations for a marked vertex on the complete graph of $N$ vertices by repeatedly querying an oracle that flips the amplitude at the marked vertex, scattering by a "coin" flip, and hopping. Physically, however, potential energy barriers can hinder the hop and cause the search to fail, even when the amplitude of not hopping decreases with $N$. We correct for these errors by interpreting the quantum walk search as an amplitude amplification algorithm and modifying the phases applied by the coin flip and oracle such that the amplification recovers the $\Theta(\sqrt{N})$ runtime.

Nuclear and High Energy PhysicsQuantum PhysicsTheoryofComputation_COMPUTATIONBYABSTRACTDEVICESComplete graphGeneral Physics and AstronomyFOS: Physical sciencesTheoryofComputation_GENERALStatistical and Nonlinear PhysicsOracleTheoretical Computer ScienceVertex (geometry)CombinatoricsAmplitudeComputational Theory and MathematicsAmplitude amplificationTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITYGrover's algorithmQuantum algorithmQuantum walkQuantum Physics (quant-ph)Mathematical PhysicsMathematicsMathematicsofComputing_DISCRETEMATHEMATICS
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Search for heavy neutral lepton production in K+ decays

2018

A search for heavy neutral lepton production in $K^+$ decays using a data sample collected with a minimum bias trigger by the NA62 experiment at CERN in 2015 is reported. Upper limits at the $10^{-7}$ to $10^{-6}$ level are established on the elements of the extended neutrino mixing matrix $|U_{\ell 4}|^2$ ($\ell=e,\mu$) for heavy neutral lepton mass in the range $170-448~{\rm MeV}/c^2$. This improves on the results from previous production searches in $K^+$ decays, setting more stringent limits and extending the mass range.

Nuclear and High Energy PhysicsleptonPontecorvo–Maki–Nakagawa–Sakata matrixheavy neutral leptons neutrino mixingFOS: Physical sciencesk mesonNA62 experiment01 natural sciencesneutrino mixingSettore FIS/04 - Fisica Nucleare e SubnuclearedecayHigh Energy Physics - ExperimentNuclear physicsneutrinoHigh Energy Physics - Experiment (hep-ex)Minimum biasEconomicaBounds; neutrinos; masses; testsTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITY0103 physical sciencesheavy neutral leptonslepton k meson decay neutrino010306 general physicsNuclear ExperimentPhysicsRange (particle radiation)Large Hadron Collider010308 nuclear & particles physicshep-exHigh Energy Physics::PhenomenologyAmbientalelcsh:QC1-999High Energy Physics::Experimentlcsh:PhysicsParticle Physics - ExperimentLepton
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Heuristic Algorithm for the Analysis of Fast Field Cycling (FFC) NMR Dispersion Curves

2021

Evaluation of nuclear magnetic relaxation dispersion (NMRD) curves obtained by the fast field cycling nuclear magnetic resonance (FFC-NMR) relaxometry technique is a valuable tool for analyzing the microscopic dynamics of condensed matter systems. However, quantitative data analysis involves several conceptual and practical issues. Moving forward from previous literature approaches, we propose a new analysis method, relying on the elaboration of the inverse integral transform of the NMRD curve. Our approach results in a true heuristic method, able to unambiguously individuate the dynamic domains in the system, thereby avoiding the possible introduction of any element of discretion. The anal…

Nuclear magnetic relaxationNanospongesRelaxometryMagnetic Resonance SpectroscopyField cyclingHeuristic (computer science)Settore AGR/13 - Chimica AgrariaInverseHeuristic algorithm010402 general chemistry01 natural sciencesAnalytical ChemistryFFC NMRCheeseDispersion (optics)HeuristicsAnalysis methodSettore CHIM/02 - Chimica FisicaCyclodextrinsChemistry010401 analytical chemistrySettore CHIM/06 - Chimica OrganicaIntegral transformMagnetic Resonance Imaging0104 chemical sciencesRelaxometryAlgorithmAlgorithmsAnalytical Chemistry
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Recent Hadronic Cross Section Measurements from BABAR

2019

New hadronic cross sections measured by the BABAR experiment are presented: e+e−→ π+π−π0π0, e+ e−→ π+π−η, and the kaonic channels e+e−→ KS KLπ0 , KS KLπ0π0 , KS KLη, KS K±π+π0 , KS K±π+η.

Nuclear physicsPhysicsCross section (physics)PhysicsQC1-999TheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITYHadronBaBar experimentEPJ Web of Conferences
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Study of theB−→J/ψK−π+π−decay and measurement of theB−→X(3872)K−branching fraction

2005

The authors study the decay B{sup -} {yields} J/{psi}K{sup -}{pi}{sup +}{pi}{sup -} using 117 million B{bar B} events collected at the {Upsilon}(4S) resonance with the BaBar detector at the PEP-II e{sup +}e{sup -} asymmetric-energy storage ring. They measure the branching fractions {Beta}(B{sup -} {yields} J/{psi}K{sup -} {pi}{sup +}{pi}{sup -}) = (116 {+-} 7(stat.) {+-} 9(syst.)) x 10{sup -5} and {Beta}(B{sup -} {yields} X(3872)K{sup -}) x {Beta}(X(3872) {yields} J/{psi}{pi}{sup +}{pi}{sup -}) = (1.28 {+-} 0.41) x 10{sup -5} and find the mass of the X(3872) to be 3873.4 {+-} 1.4MeV/c{sup 2}. They search for the h{sub c} narrow state in the decay B{sup -} {yields} h{sub c} K{sup -}, h{sub c…

Nuclear physicsPhysicsNuclear and High Energy PhysicsCrystallographyParticle decay010308 nuclear & particles physicsBranching fractionTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITYElectron–positron annihilation0103 physical sciences010306 general physics01 natural sciencesX(3872)Physical Review D
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NA48/62 latest results

2017

The NA62 experiment at the CERN SPS recorded in 2007 a large sample of K+ ? µ+?µ decays. A peak search in the missing mass spectrum of this decay is performed. In the absence of observed signal, the limits obtained on B(K+ ? µ+?h) and on the mixing matrix element |Uµ 4| are reported. The upgraded NA62 experiment started data taking in 2015. About 5×1011K+ decays have been recorded so far to measure the branching ratio of the K+ ? ?+?? decay. Preliminary results from the K+ ? ?+?? analysis based on about 5% of the 2016 statistics are reported.

Nuclear physicsPhysicsParticle physicsBranching fractionTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITYMass spectrumMatrix elementCreative commonsNA62 experimentParticle Physics - ExperimentSettore FIS/04 - Fisica Nucleare e SubnucleareLarge sample
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The scattering of 28.5 MeV 3 He particles by 12 C, 20 Ne and 40 A nuclei

1960

Differential cross-sections for the elastic and inelastic scattering of 28.5 MeV 3 He particles by the nuclei 12 C, 20 Ne and 40 A have been measured by means of a photographic technique. The 12 C ( 3 He, α) reaction was also observed. The elastic scattering distributions have been analyzed in terms of an optical model.

Nuclear reactionElastic scatteringPhysicsGeneral EnergyScatteringTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITYHelium-3Carbon-12Alpha particleAtomic physicsInelastic scatteringProceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences
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