0000000000157025

AUTHOR

J.a. Hernando

showing 8 related works from this author

Kalman filter tracking and vertexing in a silicon detector for neutrino physics

2002

Abstract This article describes the application of Kalman filter techniques for the tracking and vertexing of particles inside the NOMAD-STAR detector, a silicon vertex detector installed in NOMAD, one of the neutrino oscillation experiments at the CERN-SPS. The use of the Kalman filter simplifies computationally the tracking and vertex procedure for NOMAD-STAR. The alignment of NOMAD-STAR is shown as an example of the application of the Kalman filter for tracking purposes. The accuracy of the method is such that one obtains alignment residuals between 9 and 12 μm . Furthermore, a preliminary measure of the impact parameter (with an RMS ∼36 μm ) illustrates the vertexing capabilities of thi…

PhysicsNuclear and High Energy PhysicsParticle physicsbusiness.industryPhysics::Instrumentation and DetectorsDetectorHigh Energy Physics::PhenomenologyFísicaKalman filterTracking (particle physics)Particle detectorSemiconductor detectorNeutrino detectorComputer visionFast Kalman filterHigh Energy Physics::ExperimentArtificial intelligenceDetectors and Experimental TechniquesNeutrino oscillationbusinessInstrumentation
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A neutrino apparatus with improved capabilities for a short baseline νμ(νe) ↔ ντ search

1995

Abstract We propose the conceptual design of a Neutrino ApparatUS with Improved CApAbilities (NAUSICAA). This detector could be used for a new, short-baseline, high sensitivity νμ(νe) ↔ ντ oscillation search experiment at the CERN-SPS neutrino beam, as well as at the future Fermilab Main Injector neutrino beam. The heart of the detector is a finely instrumented target, made of a sandwich of a light Z material and high resolution tracking detectors. Downstream of the target there are tracking detectors for momentum measurement, followed by a compensating calorimeter. All these systems are contained within magnet providing a magnetic field of about 1 T. Following the magnet there is a muon de…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderCalorimeter (particle physics)Physics::Instrumentation and DetectorsMonte Carlo methodDetectorTracking (particle physics)Nuclear physicsPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentFermilabDetectors and Experimental TechniquesNeutrinoNeutrino oscillationInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Performance of long modules of silicon microstrip detectors

1998

This note describes the performance of modules assembled with up to twelve silicon microstrip detectors. These modules were built for the instrumented Silicon Target (STAR) that has been installed in the NOMAD spectrometer. Laboratory and test beam results are compared with model predictions. For a module of nine detectors, test beam results indicate a signal--to--noise ratio of 19, a hit finding efficiency of 99.8\% and a spatial resolution of 6.0 $\mu$m. Laboratory measurements indicate that modules of twelve detectors exhibit a signal--to--noise ratio of the order of 16.

PhysicsNuclear and High Energy PhysicsSpectrometerSiliconbusiness.industryPhysics::Instrumentation and DetectorsDetectorchemistry.chemical_elementFísicaParticle detectorSemiconductor detectorNuclear physicssilicon microstrip detectors; neutrino oscillationsSignal-to-noise ratioOpticschemistryMeasuring instrumentHigh Energy Physics::ExperimentDetectors and Experimental TechniquesbusinessInstrumentationImage resolution
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“RecPack” a reconstruction toolkit

2004

We present a C++ toolkit to do tracking and vertex reconstruction. The toolkit incorporates common fitting methods, as the Kalman Filter, a framework to define a detector setup, a general navigation and a simple simulation. Furthermore, the toolkit provides a collection of interfaces which facilitates the addition of new fitting methods, trajectory models, geometrical objects, pattern recognition logic, etc. Although the toolkit was originally developed to be used in High Energy Physics, it could be applied to other fields.

PhysicsNuclear and High Energy PhysicsVertex (computer graphics)Fitting methodsSimple (abstract algebra)DetectorPattern recognition (psychology)TrajectoryKalman filterTracking (particle physics)InstrumentationComputational scienceNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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A $B_4C$-silicon target for the detection of neutrino interactions

1998

This note describes the construction of a target for neutrino interactions composed of passive boron carbide plates interleaved with silicon microstrip detectors. The target contains four layers of passive material with a total mass of 45 kg and 600 single--sided silicon microstrip detectors with a total surface of 1.14 m$^2$ distributed over five layers. It is installed in the NOMAD spectrometer at the CERN SPS neutrino beam. During the 1997 run about 8000 \nm\ charged current interactions were estimated to have occurred in the target. For these events it will be possible to perform a precise measurement of both vertex and kinematical variables. This will provide invaluable experience towa…

PhysicsNuclear and High Energy PhysicsLarge Hadron ColliderSpectrometerSiliconPhysics::Instrumentation and DetectorsFísicachemistry.chemical_elementsilicon microstrip detectors; neutrino oscillations; silicon strip sensors; tracking detectors; search; alignmentNuclear physicsNeutrino detectorchemistryMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationInstrumentationCharged currentParticle Physics - Experiment
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Performance of the NOMAD-STAR detector

2003

The NOMAD-STAR detector is a silicon vertex installed in the NOMAD spectrometer at the CERN SPS neutrino beam. It consists of four layers of a passive boron carbide target with a total mass of 45 kg and five layers of 600 single sided silicon microstrip detectors covering a total area of 1.14m^2. About 11,500 nu_mu charged current interactions were reconstructed in the fiducial volume of NOMAD-STAR from the neutrino run in 1998. The potential use of silicon detectors for nu_mu (nu_e) nu_tau oscillations depends on the observation of the tau candidates by the experimental signature of a large impact parameter, in the case of the one prong decay of the tau, or a double vertex, in the case of …

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderSiliconSpectrometer010308 nuclear & particles physicsPhysics::Instrumentation and DetectorsDetectorFísicachemistry.chemical_elementneutrino physics; silicon microstrip detectors01 natural sciencesNuclear physicschemistry0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::ExperimentDetectors and Experimental TechniquesNeutrinoImpact parameter010306 general physicsInstrumentationCharged currentSTAR detector
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Search for νμ(νe) ↔ ντ oscillations with a detector based on a emulsion-silicon target

1996

We discuss the performance of a next generation νμ(νe)↔ ντ oscillation experiment, based on a target consisting of a sandwich of nuclear emulsion layers and silicon detectors. The target would be followed by a full spectrometer for energy-momentum measurement and particle identification. A τ-enriched sample is selected in terms of vertex and kinematical criteria using the electronic spectrometer, with very high efficiency, while at the same time reducing the load of background events to be scanned by up to two orders of magnitude. Events fulfilling the selection criteria are very efficiently located and scanned in the emulsion, thanks to the very good resolution allowed by the silicon track…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderSpectrometerPhysics::Instrumentation and DetectorsDetectorMonte Carlo methodParticle identificationNuclear physicsNuclear emulsionDetectors and Experimental TechniquesNeutrino oscillationInstrumentationCharged currentNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Improved measurements of cross sections and asymmetries at the Z0 resonance

1994

During the 1992 running period of the LEP e+e- collider, the DELPHI experiment accumulated approximately 24 pb-1 of data at the Z0 peak. The decays into hadrons and charged leptons have been analysed to give values for the cross sections and leptonic forward-backward asymmetries which are significantly improved with respect to those previously published by the DELPHI collaboration. Incorporating these new data, more precise values for the Z0 resonance parameters are obtained from model-independent fits. The results are interpreted within the framework of the Standard Model, yielding for the top quark mass m(t) = 157(-48)+36(expt.)-20(+19)(Higgs) GeV, and for the effective mixing angle sin2 …

Nuclear and High Energy PhysicsParticle physicsTop quarkLUND MONTE-CARLOElectron–positron annihilationLEP-SLC ENERGIESElementary particle7. Clean energy01 natural sciencesJET FRAGMENTATIONStandard ModelPHYSICSNuclear physicsBHABHA SCATTERINGParticle decay0103 physical sciencesPROGRAM[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]RADIATIVE-CORRECTIONSZ0010306 general physicsDELPHIPhysicsLOWEST-ORDER CALCULATIONScross section010308 nuclear & particles physicsDELPHI; Bhabha scattering; cross section; Z0High Energy Physics::PhenomenologyLARGE ELECTRON POSITRON COLLIDERLUND MONTE-CARLO; ELECTRON-POSITRON COLLISIONS; LOWEST-ORDER CALCULATIONS; LEP-SLC ENERGIES; BHABHA SCATTERING; RADIATIVE-CORRECTIONS; JET FRAGMENTATION; PROGRAM; PHYSICSPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHILarge Electron–Positron ColliderHiggs bosonPARTICLE PHYSICSFísica nuclearHigh Energy Physics::ExperimentELECTRON-POSITRON COLLISIONSParticle Physics - ExperimentLepton
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